Measurement of the $$t\bar{t}$$ tt¯ production cross-section and lepton differential distributions in $$e\mu $$ eμ dilepton events from pp collisions at $$\sqrt{s}=13\,\text {TeV}$$ s=13TeV with the ATLAS detector

Bibliographic Details
Title: Measurement of the $$t\bar{t}$$ tt¯ production cross-section and lepton differential distributions in $$e\mu $$ eμ dilepton events from pp collisions at $$\sqrt{s}=13\,\text {TeV}$$ s=13TeV with the ATLAS detector
Authors: ATLAS Collaboration, G. Aad, B. Abbott, D. C. Abbott, A. Abed Abud, K. Abeling, D. K. Abhayasinghe, S. H. Abidi, O. S. AbouZeid, N. L. Abraham, H. Abramowicz, H. Abreu, Y. Abulaiti, B. S. Acharya, B. Achkar, S. Adachi, L. Adam, C. Adam Bourdarios, L. Adamczyk, L. Adamek, J. Adelman, M. Adersberger, A. Adiguzel, S. Adorni, T. Adye, A. A. Affolder, Y. Afik, C. Agapopoulou, M. N. Agaras, A. Aggarwal, C. Agheorghiesei, J. A. Aguilar-Saavedra, F. Ahmadov, W. S. Ahmed, X. Ai, G. Aielli, S. Akatsuka, T. P. A. Åkesson, E. Akilli, A. V. Akimov, K. Al Khoury, G. L. Alberghi, J. Albert, M. J. Alconada Verzini, S. Alderweireldt, M. Aleksa, I. N. Aleksandrov, C. Alexa, T. Alexopoulos, A. Alfonsi, F. Alfonsi, M. Alhroob, B. Ali, M. Aliev, G. Alimonti, S. P. Alkire, C. Allaire, B. M. M. Allbrooke, B. W. Allen, P. P. Allport, A. Aloisio, A. Alonso, F. Alonso, C. Alpigiani, A. A. Alshehri, M. Alvarez Estevez, D. Álvarez Piqueras, M. G. Alviggi, Y. Amaral Coutinho, A. Ambler, L. Ambroz, C. Amelung, D. Amidei, S. P. Amor Dos Santos, S. Amoroso, C. S. Amrouche, F. An, C. Anastopoulos, N. Andari, T. Andeen, C. F. Anders, J. K. Anders, A. Andreazza, V. Andrei, C. R. Anelli, S. Angelidakis, A. Angerami, A. V. Anisenkov, A. Annovi, C. Antel, M. T. Anthony, E. Antipov, M. Antonelli, D. J. A. Antrim, F. Anulli, M. Aoki, J. A. Aparisi Pozo, L. Aperio Bella, J. P. Araque, V. Araujo Ferraz, R. Araujo Pereira, C. Arcangeletti, A. T. H. Arce, F. A. Arduh, J-F. Arguin, S. Argyropoulos, J.-H. Arling, A. J. Armbruster, A. Armstrong, O. Arnaez, H. Arnold, Z. P. Arrubarrena Tame, G. Artoni, S. Artz, S. Asai, N. Asbah, E. M. Asimakopoulou, L. Asquith, J. Assahsah, K. Assamagan, R. Astalos, R. J. Atkin, M. Atkinson, N. B. Atlay, H. Atmani, K. Augsten, G. Avolio, R. Avramidou, M. K. Ayoub, A. M. Azoulay, G. Azuelos, H. Bachacou, K. Bachas, M. Backes, F. Backman, P. Bagnaia, M. Bahmani, H. Bahrasemani, A. J. Bailey, V. R. Bailey, J. T. Baines, M. Bajic, C. Bakalis, O. K. Baker, P. J. Bakker, D. Bakshi Gupta, S. Balaji, E. M. Baldin, P. Balek, F. Balli, W. K. Balunas, J. Balz, E. Banas, A. Bandyopadhyay, Sw. Banerjee, A. A. E. Bannoura, L. Barak, W. M. Barbe, E. L. Barberio, D. Barberis, M. Barbero, G. Barbour, T. Barillari, M-S. Barisits, J. Barkeloo, T. Barklow, R. Barnea, S. L. Barnes, B. M. Barnett, R. M. Barnett, Z. Barnovska-Blenessy, A. Baroncelli, G. Barone, A. J. Barr, L. Barranco Navarro, F. Barreiro, J. Barreiro Guimarães da Costa, S. Barsov, R. Bartoldus, G. Bartolini, A. E. Barton, P. Bartos, A. Basalaev, A. Basan, A. Bassalat, M. J. Basso, R. L. Bates, S. Batlamous, J. R. Batley, B. Batool, M. Battaglia, M. Bauce, F. Bauer, K. T. Bauer, H. S. Bawa, J. B. Beacham, T. Beau, P. H. Beauchemin, F. Becherer, P. Bechtle, H. C. Beck, H. P. Beck, K. Becker, M. Becker, C. Becot, A. Beddall, A. J. Beddall, V. A. Bednyakov, M. Bedognetti, C. P. Bee, T. A. Beermann, M. Begalli, M. Begel, A. Behera, J. K. Behr, F. Beisiegel, A. S. Bell, G. Bella, L. Bellagamba, A. Bellerive, P. Bellos, K. Beloborodov, K. Belotskiy, N. L. Belyaev, D. Benchekroun, N. Benekos, Y. Benhammou, D. P. Benjamin, M. Benoit, J. R. Bensinger, S. Bentvelsen, L. Beresford, M. Beretta, D. Berge, E. Bergeaas Kuutmann, N. Berger, B. Bergmann, L. J. Bergsten, J. Beringer, S. Berlendis, G. Bernardi, C. Bernius, F. U. Bernlochner, T. Berry, P. Berta, C. Bertella, I. A. Bertram, O. Bessidskaia Bylund, N. Besson, A. Bethani, S. Bethke, A. Betti, A. J. Bevan, J. Beyer, D. S. Bhattacharya, P. Bhattarai, R. Bi, R. M. Bianchi, O. Biebel, D. Biedermann, R. Bielski, K. Bierwagen, N. V. Biesuz, M. Biglietti, T. R. V. Billoud, M. Bindi, A. Bingul, C. Bini, S. Biondi, M. Birman, T. Bisanz, J. P. Biswal, D. Biswas, A. Bitadze, C. Bittrich, K. Bjørke, K. M. Black, T. Blazek, I. Bloch, C. Blocker, A. Blue, U. Blumenschein, G. J. Bobbink, V. S. Bobrovnikov, S. S. Bocchetta, A. Bocci, D. Boerner, D. Bogavac, A. G. Bogdanchikov, C. Bohm, V. Boisvert, P. Bokan, T. Bold, A. S. Boldyrev, A. E. Bolz, M. Bomben, M. Bona, J. S. Bonilla, M. Boonekamp, C. D. Booth, H. M. Borecka-Bielska, A. Borisov, G. Borissov, J. Bortfeldt, D. Bortoletto, D. Boscherini, M. Bosman, J. D. Bossio Sola, K. Bouaouda, J. Boudreau, E. V. Bouhova-Thacker, D. Boumediene, S. K. Boutle, A. Boveia, J. Boyd, D. Boye, I. R. Boyko, A. J. Bozson, J. Bracinik, N. Brahimi, G. Brandt, O. Brandt, F. Braren, B. Brau, J. E. Brau, W. D. Breaden Madden, K. Brendlinger, L. Brenner, R. Brenner, S. Bressler, B. Brickwedde, D. L. Briglin, D. Britton, D. Britzger, I. Brock, R. Brock, G. Brooijmans, W. K. Brooks, E. Brost, J. H. Broughton, P. A. Bruckman de Renstrom, D. Bruncko, A. Bruni, G. Bruni, L. S. Bruni, S. Bruno, M. Bruschi, N. Bruscino, P. Bryant, L. Bryngemark, T. Buanes, Q. Buat, P. Buchholz, A. G. Buckley, I. A. Budagov, M. K. Bugge, F. Bührer, O. Bulekov, T. J. Burch, S. Burdin, C. D. Burgard, A. M. Burger, B. Burghgrave, J. T. P. Burr, C. D. Burton, J. C. Burzynski, V. Büscher, E. Buschmann, P. J. Bussey, J. M. Butler, C. M. Buttar, J. M. Butterworth, P. Butti, W. Buttinger, C. J. Buxo Vazquez, A. Buzatu, A. R. Buzykaev, G. Cabras, S. Cabrera Urbán, D. Caforio, H. Cai, V. M. M. Cairo, O. Cakir, N. Calace, P. Calafiura, A. Calandri, G. Calderini, P. Calfayan, G. Callea, L. P. Caloba, A. Caltabiano, S. Calvente Lopez, D. Calvet, S. Calvet, T. P. Calvet, M. Calvetti, R. Camacho Toro, S. Camarda, D. Camarero Munoz, P. Camarri, D. Cameron, R. Caminal Armadans, C. Camincher, S. Campana, M. Campanelli, A. Camplani, A. Campoverde, V. Canale, A. Canesse, M. Cano Bret, J. Cantero, T. Cao, Y. Cao, M. D. M. Capeans Garrido, M. Capua, R. Cardarelli, F. Cardillo, G. Carducci, I. Carli, T. Carli, G. Carlino, B. T. Carlson, L. Carminati, R. M. D. Carney, S. Caron, E. Carquin, S. Carrá, J. W. S. Carter, M. P. Casado, A. F. Casha, D. W. Casper, R. Castelijn, F. L. Castillo, V. Castillo Gimenez, N. F. Castro, A. Catinaccio, J. R. Catmore, A. Cattai, V. Cavaliere, E. Cavallaro, M. Cavalli-Sforza, V. Cavasinni, E. Celebi, F. Ceradini, L. Cerda Alberich, K. Cerny, A. S. Cerqueira, A. Cerri, L. Cerrito, F. Cerutti, A. Cervelli, S. A. Cetin, Z. Chadi, D. Chakraborty, W. S. Chan, W. Y. Chan, J. D. Chapman, B. Chargeishvili, D. G. Charlton, T. P. Charman, C. C. Chau, S. Che, S. Chekanov, S. V. Chekulaev, G. A. Chelkov, M. A. Chelstowska, B. Chen, C. Chen, C. H. Chen, H. Chen, J. Chen, S. Chen, S. J. Chen, X. Chen, Y-H. Chen, H. C. Cheng, H. J. Cheng, A. Cheplakov, E. Cheremushkina, R. Cherkaoui El Moursli, E. Cheu, K. Cheung, T. J. A. Chevalérias, L. Chevalier, V. Chiarella, G. Chiarelli, G. Chiodini, A. S. Chisholm, A. Chitan, I. Chiu, Y. H. Chiu, M. V. Chizhov, K. Choi, A. R. Chomont, S. Chouridou, Y. S. Chow, M. C. Chu, X. Chu, J. Chudoba, A. J. Chuinard, J. J. Chwastowski, L. Chytka, D. Cieri, K. M. Ciesla, D. Cinca, V. Cindro, I. A. Cioară, A. Ciocio, F. Cirotto, Z. H. Citron, M. Citterio, D. A. Ciubotaru, B. M. Ciungu, A. Clark, M. R. Clark, P. J. Clark, C. Clement, Y. Coadou, M. Cobal, A. Coccaro, J. Cochran, H. Cohen, A. E. C. Coimbra, L. Colasurdo, B. Cole, A. P. Colijn, J. Collot, P. Conde Muiño, S. H. Connell, I. A. Connelly, S. Constantinescu, F. Conventi, A. M. Cooper-Sarkar, F. Cormier, K. J. R. Cormier, L. D. Corpe, M. Corradi, E. E. Corrigan, F. Corriveau, A. Cortes-Gonzalez, M. J. Costa, F. Costanza, D. Costanzo, G. Cowan, J. W. Cowley, J. Crane, K. Cranmer, S. J. Crawley, R. A. Creager, S. Crépé-Renaudin, F. Crescioli, M. Cristinziani, V. Croft, G. Crosetti, A. Cueto, T. Cuhadar Donszelmann, A. R. Cukierman, W. R. Cunningham, S. Czekierda, P. Czodrowski, M. J. Da Cunha Sargedas De Sousa, J. V. Da Fonseca Pinto, C. Da Via, W. Dabrowski, F. Dachs, T. Dado, S. Dahbi, T. Dai, C. Dallapiccola, M. Dam, G. D’amen, V. D’Amico, J. Damp, J. R. Dandoy, M. F. Daneri, N. P. Dang, N. S. Dann, M. Danninger, V. Dao, G. Darbo, O. Dartsi, A. Dattagupta, T. Daubney, S. D’Auria, C. David, T. Davidek, D. R. Davis, I. Dawson, K. De, R. De Asmundis, M. De Beurs, S. De Castro, S. De Cecco, N. De Groot, P. de Jong, H. De la Torre, A. De Maria, D. De Pedis, A. De Salvo, U. De Sanctis, M. De Santis, A. De Santo, K. De Vasconcelos Corga, J. B. De Vivie De Regie, C. Debenedetti, D. V. Dedovich, A. M. Deiana, J. Del Peso, Y. Delabat Diaz, D. Delgove, F. Deliot, C. M. Delitzsch, M. Della Pietra, D. Della Volpe, A. Dell’Acqua, L. Dell’Asta, M. Delmastro, C. Delporte, P. A. Delsart, D. A. DeMarco, S. Demers, M. Demichev, G. Demontigny, S. P. Denisov, L. D’Eramo, D. Derendarz, J. E. Derkaoui, F. Derue, P. Dervan, K. Desch, C. Deterre, K. Dette, C. Deutsch, M. R. Devesa, P. O. Deviveiros, A. Dewhurst, F. A. Di Bello, A. Di Ciaccio, L. Di Ciaccio, W. K. Di Clemente, C. Di Donato, A. Di Girolamo, G. Di Gregorio, B. Di Micco, R. Di Nardo, K. F. Di Petrillo, R. Di Sipio, D. Di Valentino, C. Diaconu, F. A. Dias, T. Dias Do Vale, M. A. Diaz, J. Dickinson, E. B. Diehl, J. Dietrich, S. Díez Cornell, A. Dimitrievska, W. Ding, J. Dingfelder, F. Dittus, F. Djama, T. 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Zakareishvili, N. Zakharchuk, S. Zambito, D. Zanzi, D. R. Zaripovas, S. V. Zeißner, C. Zeitnitz, G. Zemaityte, J. C. Zeng, O. Zenin, T. Ženiš, D. Zerwas, M. Zgubič, B. Zhang, D. F. Zhang, G. Zhang, H. Zhang, J. Zhang, L. Zhang, M. Zhang, R. Zhang, S. Zhang, X. Zhang, Y. Zhang, Z. Zhang, P. Zhao, Y. Zhao, Z. Zhao, A. Zhemchugov, Z. Zheng, D. Zhong, B. Zhou, C. Zhou, M. S. Zhou, M. Zhou, N. Zhou, Y. Zhou, C. G. Zhu, C. Zhu, H. L. Zhu, H. Zhu, J. Zhu, Y. Zhu, X. Zhuang, K. Zhukov, V. Zhulanov, D. Zieminska, N. I. Zimine, S. Zimmermann, Z. Zinonos, M. Ziolkowski, L. Živković, G. Zobernig, A. Zoccoli, K. Zoch, T. G. Zorbas, R. Zou, L. Zwalinski
Source: European Physical Journal C: Particles and Fields, Vol 80, Iss 6, Pp 1-70 (2020)
Publisher Information: SpringerOpen, 2020.
Publication Year: 2020
Collection: LCC:Astrophysics
LCC:Nuclear and particle physics. Atomic energy. Radioactivity
Subject Terms: Astrophysics, QB460-466, Nuclear and particle physics. Atomic energy. Radioactivity, QC770-798
More Details: Abstract The inclusive top quark pair ($$t\bar{t}$$ tt¯ ) production cross-section $$\sigma _{t\bar{t}}$$ σtt¯ has been measured in proton–proton collisions at $$\sqrt{s}=13\,\text {TeV}$$ s=13TeV , using 36.1 fb$$^{-1}$$ -1 of data collected in 2015–2016 by the ATLAS experiment at the LHC. Using events with an opposite-charge $$e\mu $$ eμ pair and b-tagged jets, the cross-section is measured to be: $$\begin{aligned} \sigma _{t\bar{t}} = 826.4 \pm 3.6\,\mathrm {(stat)}\ \pm 11.5\,\mathrm {(syst)}\ \pm 15.7\,\mathrm {(lumi)}\ \pm 1.9\,\mathrm {(beam)}\,\mathrm {pb}, \end{aligned}$$ σtt¯=826.4±3.6(stat)±11.5(syst)±15.7(lumi)±1.9(beam)pb, where the uncertainties reflect the limited size of the data sample, experimental and theoretical systematic effects, the integrated luminosity, and the LHC beam energy, giving a total uncertainty of 2.4%. The result is consistent with theoretical QCD calculations at next-to-next-to-leading order. It is used to determine the top quark pole mass via the dependence of the predicted cross-section on $$m_t^{\mathrm{pole}}$$ mtpole , giving $$m_t^{\mathrm{pole}}=173.1^{+2.0}_{-2.1}\,\text {GeV}$$ mtpole=173.1-2.1+2.0GeV . It is also combined with measurements at $$\sqrt{s}=7\,\text {TeV}$$ s=7TeV and $$\sqrt{s}=8\,\text {TeV}$$ s=8TeV to derive ratios and double ratios of $$t\bar{t}$$ tt¯ and Z cross-sections at different energies. The same event sample is used to measure absolute and normalised differential cross-sections as functions of single-lepton and dilepton kinematic variables, and the results are compared with predictions from various Monte Carlo event generators.
Document Type: article
File Description: electronic resource
Language: English
ISSN: 1434-6044
1434-6052
Relation: http://link.springer.com/article/10.1140/epjc/s10052-020-7907-9; https://doaj.org/toc/1434-6044; https://doaj.org/toc/1434-6052
DOI: 10.1140/epjc/s10052-020-7907-9
Access URL: https://doaj.org/article/b75d565816a64c408609a2f7ae9e8643
Accession Number: edsdoj.b75d565816a64c408609a2f7ae9e8643
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  Value: <anid>AN0144642803;c7g01jun.20;2020Jul20.08:15;v2.2.500</anid> <title id="AN0144642803-1">Measurement of the tt¯ production cross-section and lepton differential distributions in eμ dilepton events from pp collisions at s=13TeV with the ATLAS detector </title> <sbt id="AN0144642803-2">Introduction</sbt> <p>The inclusive top quark pair ( t t ¯ ) production cross-section σ t t ¯ has been measured in proton–proton collisions at s = 13 TeV , using 36.1 fb - 1 of data collected in 2015–2016 by the ATLAS experiment at the LHC. Using events with an opposite-charge e μ pair and b-tagged jets, the cross-section is measured to be: σ t t ¯ = 826.4 ± 3.6 (stat) ± 11.5 (syst) ± 15.7 (lumi) ± 1.9 (beam) pb , where the uncertainties reflect the limited size of the data sample, experimental and theoretical systematic effects, the integrated luminosity, and the LHC beam energy, giving a total uncertainty of 2.4%. The result is consistent with theoretical QCD calculations at next-to-next-to-leading order. It is used to determine the top quark pole mass via the dependence of the predicted cross-section on m t pole , giving m t pole = 173. 1 - 2.1 + 2.0 GeV . It is also combined with measurements at s = 7 TeV and s = 8 TeV to derive ratios and double ratios of t t ¯ and Z cross-sections at different energies. The same event sample is used to measure absolute and normalised differential cross-sections as functions of single-lepton and dilepton kinematic variables, and the results are compared with predictions from various Monte Carlo event generators.</p> <p>The study of top quark–antiquark ( <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> ) production forms a cornerstone of the physics programme of the ATLAS experiment at the CERN Large Hadron Collider (LHC), allowing quantum chromodynamics (QCD) to be probed at some of the highest accessible energy scales. The large mass of the top quark, close to the scale of electroweak symmetry breaking, gives it a unique role in the Standard Model of particle physics and potential extensions, and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> production also forms an important background in many searches for physics beyond the Standard Model. Precise measurements of absolute rates and differential distributions in <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> production are therefore a vital tool in fully exploiting the discovery potential of the LHC.</p> <p>Predictions for the inclusive <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> production cross-section in proton–proton (<emph>pp</emph>) collisions, <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> , are available at next-to-next-to-leading-order (NNLO) accuracy in the strong coupling constant <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>α</mi><mi mathvariant="normal">S</mi></msub></math> </ephtml> , including the resummation of next-to-next-to-leading logarithmic (NNLL) soft gluon terms [[<reflink idref="bib1" id="ref1">1</reflink>]–[<reflink idref="bib6" id="ref2">6</reflink>]], and are in excellent agreement with measurements from ATLAS and CMS at <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>7</mn></mrow></math> </ephtml> , 8 and 13 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> [[<reflink idref="bib7" id="ref3">7</reflink>]–[<reflink idref="bib13" id="ref4">13</reflink>]]. At <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> , and assuming a fixed top quark mass of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>m</mi><mi>t</mi></msub><mo>=</mo><mn>172.5</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math> </ephtml> , the NNLO+NNLL prediction is <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mn>832</mn><mo>±</mo><msubsup><mn>35</mn><mrow><mo>-</mo><mn>29</mn></mrow><mrow><mo>+</mo><mn>20</mn></mrow></msubsup></mrow></math> </ephtml> pb, as calculated using the Top++ 2.0 program [[<reflink idref="bib14" id="ref5">14</reflink>]]. The first uncertainty corresponds to parton distribution function (PDF) and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>α</mi><mi mathvariant="normal">S</mi></msub></math> </ephtml> uncertainties, and the second to QCD scale variations. The former were calculated using the PDF4LHC prescription [[<reflink idref="bib15" id="ref6">15</reflink>]] with the MSTW2008 [[<reflink idref="bib16" id="ref7">16</reflink>]], CT10 NNLO [[<reflink idref="bib18" id="ref8">18</reflink>]] and NNPDF2.3 5f FFN [[<reflink idref="bib20" id="ref9">20</reflink>]] PDF sets.[<reflink idref="bib1" id="ref10">1</reflink>] The latter was calculated from the envelope of predictions with the QCD renormalisation and factorisation scales varied independently up or down by a factor of two from their default values of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>μ</mi><mi mathvariant="normal">F</mi></msub><mo>=</mo><msub><mi>μ</mi><mi mathvariant="normal">R</mi></msub><mo>=</mo><msub><mi>m</mi><mi>t</mi></msub></mrow></math> </ephtml> , whilst never letting them differ by more than a factor of two [[<reflink idref="bib21" id="ref11">21</reflink>]]. The total uncertainty corresponds to a relative precision of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msubsup><mrow /><mrow><mo>-</mo><mn>5.5</mn></mrow><mrow><mo>+</mo><mn>4.8</mn></mrow></msubsup><mo>%</mo></mrow></math> </ephtml> .</p> <p>The predicted cross-section also depends strongly on <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>m</mi><mi>t</mi></msub></math> </ephtml> , decreasing by 2.7% for a 1 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> increase in the top mass. The top quark mass parameter used in the cross-section prediction is actually the pole mass <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>m</mi><mi>t</mi><mi mathvariant="normal">pole</mi></msubsup></math> </ephtml> , corresponding to the definition of the mass of a free particle. This allows <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> measurements to be interpreted as measurements of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>m</mi><mi>t</mi><mi mathvariant="normal">pole</mi></msubsup></math> </ephtml> , free of the theoretical ambiguities linked to the direct reconstruction of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>m</mi><mi>t</mi></msub></math> </ephtml> from the invariant mass of its decay products [[<reflink idref="bib23" id="ref12">23</reflink>]–[<reflink idref="bib26" id="ref13">26</reflink>]]. Ratios of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> production cross-sections at different centre-of-mass energies are also of interest, e.g. <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msubsup><mi>R</mi><mrow><mn>13</mn><mo stretchy="false">/</mo><mn>7</mn></mrow><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msubsup><mo>=</mo><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub><mrow><mo stretchy="false">(</mo><mn>13</mn><mspace width="0.166667em" /><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow><mo stretchy="false">)</mo></mrow><mo stretchy="false">/</mo><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub><mrow><mo stretchy="false">(</mo><mn>7</mn><mspace width="0.166667em" /><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow><mo stretchy="false">)</mo></mrow></mrow></math> </ephtml> . Predictions for such ratios benefit from significant cancellations in the QCD scale and top quark mass uncertainties, but are still sensitive to the choice of PDF. The NNLO+NNLL predictions with the same set of assumptions as given for <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> above, and a 1 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> uncertainty in <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>m</mi><mi>t</mi></msub></math> </ephtml> , are <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msubsup><mi>R</mi><mrow><mn>13</mn><mo stretchy="false">/</mo><mn>7</mn></mrow><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msubsup><mo>=</mo><mn>4.69</mn><mo>±</mo><mn>0.16</mn></mrow></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msubsup><mi>R</mi><mrow><mn>13</mn><mo stretchy="false">/</mo><mn>8</mn></mrow><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msubsup><mo>=</mo><mn>3.28</mn><mo>±</mo><mn>0.08</mn></mrow></math> </ephtml> , i.e. relative uncertainties of 3.3% and 2.5%. Double ratios of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> to <emph>Z</emph> production cross-sections allow the experimental uncertainties to be further reduced, by normalising the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> cross-section at each energy to the corresponding cross-section for <emph>Z</emph> boson production [[<reflink idref="bib27" id="ref14">27</reflink>]].</p> <p>Within the Standard Model, the top quark decays 99.8% of the time to a <emph>W</emph> boson and <emph>b</emph>-quark [[<reflink idref="bib28" id="ref15">28</reflink>]], making the final-state topologies in <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> production dependent on the decay modes of the <emph>W</emph> bosons. The channel with an electron–muon pair with opposite electric charges, i.e. <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo stretchy="false">→</mo><msup><mi>W</mi><mo>+</mo></msup><mi>b</mi><msup><mi>W</mi><mo>-</mo></msup><mover accent="true"><mrow><mi>b</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo stretchy="false">→</mo><msup><mi>e</mi><mo>+</mo></msup><msup><mi>μ</mi><mo>-</mo></msup><mi>ν</mi><mover accent="true"><mrow><mi>ν</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mi>b</mi><mover accent="true"><mrow><mi>b</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> , is particularly clean.[<reflink idref="bib2" id="ref16">2</reflink>] It was exploited to make the most precise ATLAS measurements of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> at <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>7</mn></mrow></math> </ephtml> , 8 and 13 TeV [[<reflink idref="bib7" id="ref17">7</reflink>], [<reflink idref="bib9" id="ref18">9</reflink>]], based on events with an opposite-sign <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>e</mi><mi>μ</mi></mrow></math> </ephtml> pair and one or two jets tagged as likely to contain <emph>b</emph>-hadrons (<emph>b</emph>-tagged). The <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> measurement in Ref. [[<reflink idref="bib9" id="ref19">9</reflink>]] was based on the 3.2 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mspace width="0.333333em" /><mtext>fb</mtext><msup><mspace width="0.333333em" /><mrow><mo>-</mo><mn>1</mn></mrow></msup></mrow></math> </ephtml> dataset recorded in 2015. This paper describes a new measurement of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> at <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> using the same final state, but applied to the combined 2015–2016 ATLAS dataset of 36.1 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mspace width="0.333333em" /><mtext>fb</mtext><msup><mspace width="0.333333em" /><mrow><mo>-</mo><mn>1</mn></mrow></msup></mrow></math> </ephtml> . The cross-section measurement is further used to determine the top quark pole mass via the dependence of the prediction on <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>m</mi><mi>t</mi><mi mathvariant="normal">pole</mi></msubsup></math> </ephtml> , complementing the analogous measurement with the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>7</mn></mrow></math> </ephtml> and 8 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> data [[<reflink idref="bib7" id="ref20">7</reflink>]]. This paper also updates the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> cross-section ratios <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>R</mi><mrow><mn>13</mn><mo stretchy="false">/</mo><mn>7</mn></mrow><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msubsup></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>R</mi><mrow><mn>13</mn><mo stretchy="false">/</mo><mn>8</mn></mrow><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msubsup></math> </ephtml> , the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo stretchy="false">/</mo><mi>Z</mi></mrow></math> </ephtml> ratio <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>R</mi><mn>13</mn><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo stretchy="false">/</mo><mi>Z</mi></mrow></msubsup></math> </ephtml> , and the double ratios of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> to <emph>Z</emph> cross-sections <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>R</mi><mrow><mn>13</mn><mo stretchy="false">/</mo><mn>7</mn></mrow><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo stretchy="false">/</mo><mi>Z</mi></mrow></msubsup></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>R</mi><mrow><mn>13</mn><mo stretchy="false">/</mo><mn>8</mn></mrow><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo stretchy="false">/</mo><mi>Z</mi></mrow></msubsup></math> </ephtml> , using the new <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> result, superseding those derived from the previous <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> measurement in Ref. [[<reflink idref="bib27" id="ref21">27</reflink>]].</p> <p>The <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>e</mi><mi>μ</mi><mo>+</mo><mi>b</mi></mrow></math> </ephtml> -tagged jets sample also allows precise measurements of the differential distributions of the leptons produced in <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> events to be made. ATLAS has published [[<reflink idref="bib29" id="ref22">29</reflink>]] measurements at <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>8</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> of the absolute and normalised differential cross-sections as functions of the transverse momentum <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>ℓ</mi></msubsup></math> </ephtml> and absolute pseudorapidity <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>η</mi><mi>ℓ</mi></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> of the single leptons[<reflink idref="bib3" id="ref23">3</reflink>] (combined for electrons and muons), the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> , invariant mass and absolute rapidity of the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>e</mi><mi>μ</mi></mrow></math> </ephtml> system ( <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mrow><mi>e</mi><mi>μ</mi></mrow></msubsup></math> </ephtml> , <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>y</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> ), the absolute azimuthal angle <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mo stretchy="false">|</mo><mi mathvariant="normal">Δ</mi><mi>ϕ</mi><mo stretchy="false">|</mo></mrow></math> </ephtml> between the two leptons in the transverse plane ( <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi mathvariant="normal">Δ</mi><msup><mi>ϕ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math> </ephtml> ), and the scalar sums of the transverse momenta ( <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>e</mi></msubsup><mo>+</mo><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>μ</mi></msubsup></mrow></math> </ephtml> ) and energies ( <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msup><mi>E</mi><mi>e</mi></msup><mo>+</mo><msup><mi>E</mi><mi>μ</mi></msup></mrow></math> </ephtml> ) of the two leptons. These distributions were found to be generally well described by predictions from a variety of leading-order (LO) multileg and next-to-leading-order (NLO) <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> matrix-element event generators interfaced to parton showers, and by NLO fixed-order QCD calculations. The sensitivity of the data to the gluon PDF and to the top quark pole mass was also demonstrated. This paper measures the same distributions at <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> , using <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> samples which are about six times the size of those available at <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>8</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> . Two-dimensional distributions of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>η</mi><mi>ℓ</mi></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> , <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>y</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi mathvariant="normal">Δ</mi><msup><mi>ϕ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math> </ephtml> as functions of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></math> </ephtml> are also reported. The data are again compared with the predictions of various NLO <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> matrix-element event generators, but the interpretations in terms of PDF constraints and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>m</mi><mi>t</mi><mi mathvariant="normal">pole</mi></msubsup></math> </ephtml> are left for future work.</p> <p>The event selection, measurement methodology and uncertainty evaluations for both the inclusive <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> cross-section and the differential distributions are similar to those used at <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>7</mn></mrow></math> </ephtml> and 8 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> [[<reflink idref="bib7" id="ref24">7</reflink>], [<reflink idref="bib29" id="ref25">29</reflink>]], with the exception that the minimum lepton transverse momentum requirement has been lowered from 25 to 20 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> , whilst still requiring at least one lepton to be above the lepton trigger threshold of 21–27 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> . This increases the fraction of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo stretchy="false">→</mo><mi>e</mi><mi>μ</mi><mi>ν</mi><mover accent="true"><mrow><mi>ν</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mi>b</mi><mover accent="true"><mrow><mi>b</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> events that are selected by 16%, thus reducing the extrapolation uncertainties in the modelling of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> production and decay. The data and Monte Carlo simulation samples used in the analyses are described in Sect. 2, followed by the event reconstruction and selection in Sect. 3. The measurement methodology for both the inclusive and differential cross-sections is described in Sect. 4, and the evaluation of systematic uncertainties in Sect. 5. The inclusive cross-section results are given in Sect. 6, together with the derivation of the top quark pole mass from <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> , and the corresponding <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo stretchy="false">/</mo><mi>Z</mi></mrow></math> </ephtml> cross-section ratios. The differential cross-section results are discussed in Sect. 7, and compared with the predictions of several <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> event generators. Finally, conclusions are discussed in Sect. 8.</p> <hd id="AN0144642803-3">Data and simulated event samples</hd> <p>The ATLAS detector [[<reflink idref="bib30" id="ref26">30</reflink>]–[<reflink idref="bib32" id="ref27">32</reflink>]] at the LHC covers nearly the entire solid angle around the collision point. It consists of an inner tracking detector surrounded by a thin superconducting solenoid producing a 2T axial magnetic field, electromagnetic and hadronic calorimeters, and an external muon spectrometer incorporating three large toroidal magnet assemblies. The analysis was performed on samples of proton–proton collision data collected at <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> in 2015 and 2016, corresponding to total integrated luminosities of 3.2 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mspace width="0.333333em" /><mtext>fb</mtext><msup><mspace width="0.333333em" /><mrow><mo>-</mo><mn>1</mn></mrow></msup></mrow></math> </ephtml> in 2015 and 32.9 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mspace width="0.333333em" /><mtext>fb</mtext><msup><mspace width="0.333333em" /><mrow><mo>-</mo><mn>1</mn></mrow></msup></mrow></math> </ephtml> in 2016 after data quality requirements. Events were required to pass a single-electron or single-muon trigger [[<reflink idref="bib33" id="ref28">33</reflink>]], with transverse momentum thresholds that were progressively raised during the data-taking as the instantaneous luminosity increased. The electron trigger was fully efficient for electrons with reconstructed <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub><mo>></mo><mn>25</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math> </ephtml> in 2015 and the first 6 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mspace width="0.333333em" /><mtext>fb</mtext><msup><mspace width="0.333333em" /><mrow><mo>-</mo><mn>1</mn></mrow></msup></mrow></math> </ephtml> of 2016 data, and for <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub><mo>></mo><mn>27</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math> </ephtml> for the remainder. The corresponding muon trigger thresholds were <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub><mo>></mo><mn>21</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math> </ephtml> for 2015 data, <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub><mo>></mo><mn>25</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math> </ephtml> for the first 6 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mspace width="0.333333em" /><mtext>fb</mtext><msup><mspace width="0.333333em" /><mrow><mo>-</mo><mn>1</mn></mrow></msup></mrow></math> </ephtml> of 2016 data and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub><mo>></mo><mn>27</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math> </ephtml> for the rest. Each triggered event also includes the signals from on average 14 (<reflink idref="bib25" id="ref29">25</reflink>) additional inelastic <emph>pp</emph> collisions in 2015 (2016) data, referred to as pileup.</p> <p>Monte Carlo simulated event samples were used to develop the analysis procedures, to evaluate signal and background contributions, and to compare with data. Samples were processed using either the full ATLAS detector simulation [[<reflink idref="bib35" id="ref30">35</reflink>]] based on GEANT4 [[<reflink idref="bib36" id="ref31">36</reflink>]], or with a faster simulation making use of parameterised showers in the calorimeters [[<reflink idref="bib37" id="ref32">37</reflink>]]. The effects of pileup were simulated by generating additional inelastic <emph>pp</emph> collisions with Pythia8 (v8.186) [[<reflink idref="bib38" id="ref33">38</reflink>]] using the A2 set of parameter values (tune) [[<reflink idref="bib39" id="ref34">39</reflink>]] and overlaying them on the primary simulated events. These combined events were then processed using the same reconstruction and analysis chain as the data. Small corrections were applied to lepton trigger and reconstruction efficiencies to improve agreement with the response observed in data.</p> <p>The baseline simulated <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> sample was produced using the NLO matrix-element event generator Powheg-Box v2 (referred to hereafter as Powheg) [[<reflink idref="bib40" id="ref35">40</reflink>]–[<reflink idref="bib43" id="ref36">43</reflink>]] with the NNPDF3.0 NLO PDF set [[<reflink idref="bib44" id="ref37">44</reflink>]], interfaced to Pythia8 (v8.210) with the NNPDF2.3 LO PDF set and the A14 tune [[<reflink idref="bib45" id="ref38">45</reflink>]] for the parton shower, hadronisation and underlying-event modelling. In the Powheg configuration, the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>h</mi><mi mathvariant="normal">damp</mi></msub></math> </ephtml> parameter, which gives a cut-off scale for the first gluon emission, was set to <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mfrac><mn>3</mn><mn>2</mn></mfrac><msub><mi>m</mi><mi>t</mi></msub></mrow></math> </ephtml> , and the factorisation and renormalisation scales were set to <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>μ</mi><mi mathvariant="normal">F</mi></msub><mo>=</mo><msub><mi>μ</mi><mi mathvariant="normal">R</mi></msub><mo>=</mo><msqrt><mrow><mo stretchy="false">(</mo><msubsup><mi>m</mi><mrow><mi>t</mi></mrow><mn>2</mn></msubsup><mo>+</mo><msup><mrow><mo stretchy="false">(</mo><msub><mi>p</mi><mrow><mi mathvariant="normal">T</mi><mo>,</mo><mi>t</mi></mrow></msub><mo stretchy="false">)</mo></mrow><mn>2</mn></msup><mo stretchy="false">)</mo></mrow></msqrt></mrow></math> </ephtml> , where the top quark <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> is evaluated before radiation [[<reflink idref="bib46" id="ref39">46</reflink>]].</p> <p>Alternative <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> simulation samples used to assess systematic uncertainties were generated with Powheg interfaced to Herwig7 (v7.0.4) [[<reflink idref="bib47" id="ref40">47</reflink>]] with the H7UE tune, and with the MadGraph5_aMC@NLO (v2.3.3.p1) generator (referred to hereafter as aMC@NLO) [[<reflink idref="bib48" id="ref41">48</reflink>]] with the NNPDF3.0 NLO PDF set, interfaced to Pythia8 with the A14 tune. In the aMC@NLO sample, the renormalisation and factorisation scales were set in the same way as for Powheg, and the MC@NLO prescription [[<reflink idref="bib49" id="ref42">49</reflink>]] was used for matching the NLO matrix element to the parton shower. Uncertainties related to the amount of initial- and final-state radiation were explored using two alternative Powheg + Pythia8 samples: one with <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>h</mi><mi mathvariant="normal">damp</mi></msub></math> </ephtml> set to <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mn>3</mn><msub><mi>m</mi><mi>t</mi></msub></mrow></math> </ephtml> , <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>μ</mi><mi mathvariant="normal">F</mi></msub></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>μ</mi><mi mathvariant="normal">R</mi></msub></math> </ephtml> reduced by a factor of two from their default values, and the A14v3cUp tune variation, giving more parton-shower radiation; and a second sample with <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>h</mi><mi mathvariant="normal">damp</mi></msub><mo>=</mo><mfrac><mn>3</mn><mn>2</mn></mfrac><msub><mi>m</mi><mi>t</mi></msub></mrow></math> </ephtml> , <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>μ</mi><mi mathvariant="normal">F</mi></msub></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>μ</mi><mi mathvariant="normal">R</mi></msub></math> </ephtml> increased by a factor of two and the A14v3cDo tune variation, giving less parton-shower radiation. These parameter variations were chosen in order to reproduce differential cross-section and jet multiplicity distributions measured in <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> events, as discussed in Ref. [[<reflink idref="bib46" id="ref43">46</reflink>]]. The top quark mass was set to 172.5 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> in all these samples, consistent with measurements from ATLAS [[<reflink idref="bib50" id="ref44">50</reflink>]] and CMS [[<reflink idref="bib51" id="ref45">51</reflink>]]. The <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>W</mi><mo stretchy="false">→</mo><mi>ℓ</mi><mi>ν</mi></mrow></math> </ephtml> branching ratio was set to the Standard Model prediction of 0.1082 per lepton flavour [[<reflink idref="bib52" id="ref46">52</reflink>]], and the EvtGen program [[<reflink idref="bib53" id="ref47">53</reflink>]] was used to handle the decays of <emph>b</emph>- and <emph>c</emph>-flavoured hadrons. All the samples were normalised using the NNLO+NNLL inclusive cross-section prediction discussed in Sect. 1 when comparing simulation with data. Additional <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> samples with different event generator configurations were used in comparisons with the measured normalised differential cross-sections as discussed in Sect. 7.2.</p> <p>Backgrounds in these measurements are classified into two types: those with two real prompt leptons (electrons or muons) from <emph>W</emph> or <emph>Z</emph> boson decays (including those produced by leptonic decays of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mi>τ</mi></math> </ephtml> -leptons), and those where at least one of the reconstructed leptons is misidentified, i.e. a non-prompt lepton from the decay of a bottom or charm hadron, an electron from a photon conversion, a hadronic jet misidentified as an electron, or a muon produced from the decay in flight of a pion or kaon. The background with two real prompt leptons is dominated by the associated production of a <emph>W</emph> boson and single top quark, <emph>Wt</emph>. This process was simulated using Powheg v1 [[<reflink idref="bib54" id="ref48">54</reflink>]] with the CT10 NLO PDF set [[<reflink idref="bib18" id="ref49">18</reflink>]], interfaced to Pythia6 (v6.428) [[<reflink idref="bib55" id="ref50">55</reflink>]] with the P2012 tune [[<reflink idref="bib56" id="ref51">56</reflink>]]. The 'diagram removal' scheme [[<reflink idref="bib57" id="ref52">57</reflink>]] was used to handle the interference between the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> and <emph>Wt</emph> final states that occurs at NLO. The sample was normalised to a cross-section of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mn>71.7</mn><mo>±</mo><mn>3.8</mn></mrow></math> </ephtml> pb, based on the approximate NNLO calculation [[<reflink idref="bib58" id="ref53">58</reflink>]] using the MSTW2008 NNLO PDF set [[<reflink idref="bib16" id="ref54">16</reflink>]], and taking into account PDF and QCD scale uncertainties. Smaller backgrounds result from <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>Z</mi><mo stretchy="false">→</mo><mi>τ</mi><mi>τ</mi><mo stretchy="false">(</mo><mo stretchy="false">→</mo><mi>e</mi><mi>μ</mi><mo stretchy="false">)</mo></mrow></math> </ephtml> +jets, and from diboson production (<emph>WW</emph>, <emph>WZ</emph> and <emph>ZZ</emph>) in association with jets. These backgrounds were modelled using Sherpa 2.2.1 [[<reflink idref="bib60" id="ref55">60</reflink>]] (<emph>Z</emph>+jets) and Sherpa 2.1.1 (dibosons), as discussed in Ref. [[<reflink idref="bib61" id="ref56">61</reflink>]]. Production of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> in association with a leptonically decaying <emph>W</emph>, <emph>Z</emph> or Higgs boson gives a negligible contribution to the opposite-sign <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>e</mi><mi>μ</mi></mrow></math> </ephtml> samples compared to inclusive <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> production, but is significant in the same-sign control samples used to assess the background from misidentified leptons. These processes were simulated using aMC@NLO + Pythia8 ( <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo>+</mo><mi>W</mi><mo stretchy="false">/</mo><mi>Z</mi></mrow></math> </ephtml> ) or Powheg + Pythia8 ( <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo>+</mo><mi>H</mi></mrow></math> </ephtml> ) [[<reflink idref="bib61" id="ref57">61</reflink>]].</p> <p>Backgrounds with one real and one misidentified lepton arise from <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> events with one leptonically decaying and one hadronically decaying <emph>W</emph>, including <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>W</mi><mo stretchy="false">→</mo><mi>τ</mi><mi>ν</mi></mrow></math> </ephtml> with a hadronic <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mi>τ</mi></math> </ephtml> decay. These processes were simulated with Powheg + Pythia8 in the same way as for dileptonic <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> . Similar backgrounds also arise from <emph>W</emph>+jets production, modelled with Sherpa 2.2.1 as for <emph>Z</emph>+jets; and <emph>t</emph>-channel single top quark production, modelled with Powheg + Pythia6 [[<reflink idref="bib62" id="ref58">62</reflink>]] with the CT10 PDF set and P2012 tune. The contributions of these backgrounds to the opposite-sign samples were determined with the help of the same-sign control samples in data. Other backgrounds, including processes with two misidentified leptons, are negligible after the event selections used in the analysis.</p> <hd id="AN0144642803-4">Event reconstruction and selection</hd> <p>The analysis makes use of reconstructed electrons, muons and <emph>b</emph>-tagged jets. Electron candidates were reconstructed from a localised cluster of energy deposits in the electromagnetic calorimeter matched to a track in the inner detector, passing the 'Tight' likelihood-based requirement of Ref. [[<reflink idref="bib63" id="ref59">63</reflink>]]. They were required to have transverse energy <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>E</mi><mi mathvariant="normal">T</mi></msub><mo>></mo><mn>20</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math> </ephtml> and pseudorapidity <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mo stretchy="false">|</mo><mi>η</mi><mo stretchy="false">|</mo><mo><</mo><mn>2.47</mn></mrow></math> </ephtml> , excluding the transition region between the barrel and endcap electromagnetic calorimeters, <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mn>1.37</mn><mo><</mo><mo stretchy="false">|</mo><mi>η</mi><mo stretchy="false">|</mo><mo><</mo><mn>1.52</mn></mrow></math> </ephtml> . To ensure they originated from the event primary vertex, electrons were required to satisfy requirements on the transverse impact parameter significance calculated relative to the beam line of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msub><mi>d</mi><mn>0</mn></msub><mrow><mo stretchy="false">|</mo><mo stretchy="false">/</mo></mrow><msub><mi>σ</mi><msub><mi>d</mi><mn>0</mn></msub></msub><mo><</mo><mn>5</mn></mrow></math> </ephtml> , and on the longitudinal impact parameter calculated relative to the event primary vertex of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo><mi mathvariant="normal">Δ</mi></mrow><msub><mi>z</mi><mn>0</mn></msub><mrow><mo>sin</mo><mi>θ</mi><mo stretchy="false">|</mo><mo><</mo><mn>0.5</mn></mrow></mrow></math> </ephtml> mm, where <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mi>θ</mi></math> </ephtml> is the polar angle of the track. The event primary vertex was defined as the reconstructed vertex with the highest sum of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mn>2</mn></msubsup></math> </ephtml> of associated tracks. To reduce background from non-prompt electrons, candidates were further required to be isolated, using <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> - and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mo stretchy="false">|</mo><mi>η</mi><mo stretchy="false">|</mo></mrow></math> </ephtml> -dependent requirements on the summed calorimeter energy within a cone of size <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi mathvariant="normal">Δ</mi><mi>R</mi><mo>=</mo><mn>0.2</mn></mrow></math> </ephtml> around the electron cluster, and on the sum of track <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> within a cone of variable size <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi mathvariant="normal">Δ</mi><mi>R</mi><mo>=</mo><mi mathvariant="normal">min</mi><mo stretchy="false">(</mo><mn>0.2</mn><mo>,</mo><mn>10</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow><mo stretchy="false">/</mo><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub><mrow><mo stretchy="false">(</mo><mi>e</mi><mo stretchy="false">)</mo></mrow><mo stretchy="false">)</mo></mrow></math> </ephtml> around the electron track direction. The selections were tuned to give a 90% efficiency for electrons of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub><mo>=</mo><mn>25</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math> </ephtml> in simulated <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>Z</mi><mo stretchy="false">→</mo><mi>e</mi><mi>e</mi></mrow></math> </ephtml> events, rising to 99% at 60 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> .</p> <p>Muon candidates were reconstructed by combining matching tracks reconstructed in the inner detector and muon spectrometer, and were required to have <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub><mo>></mo><mn>20</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math> </ephtml> , <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mo stretchy="false">|</mo><mi>η</mi><mo stretchy="false">|</mo><mo><</mo><mn>2.5</mn></mrow></math> </ephtml> and to satisfy the 'Medium' requirements of Ref. [[<reflink idref="bib64" id="ref60">64</reflink>]]. Muons were also required to be isolated using calorimeter and track information in the same way as it was used for electrons, except that the track-based isolation was calculated with a cone of size <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi mathvariant="normal">Δ</mi><mi>R</mi><mo>=</mo><mi mathvariant="normal">min</mi><mo stretchy="false">(</mo><mn>0.3</mn><mo>,</mo><mn>10</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow><mo stretchy="false">/</mo><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub><mrow><mo stretchy="false">(</mo><mi>μ</mi><mo stretchy="false">)</mo></mrow><mo stretchy="false">)</mo></mrow></math> </ephtml> . The selections were again tuned to give efficiencies varying from 90% at <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub><mo>=</mo><mn>25</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math> </ephtml> to 99% at 60 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> on simulated <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>Z</mi><mo stretchy="false">→</mo><mi>μ</mi><mi>μ</mi></mrow></math> </ephtml> events. No requirements were made on the muon impact parameters relative to the primary vertex, as they do not provide any useful additional background rejection in this event topology.</p> <p>Jets were reconstructed using the anti- <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>k</mi><mi>t</mi></msub></math> </ephtml> algorithm [[<reflink idref="bib65" id="ref61">65</reflink>]] with radius parameter <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>R</mi><mo>=</mo><mn>0.4</mn></mrow></math> </ephtml> , starting from topological clusters in the calorimeters [[<reflink idref="bib67" id="ref62">67</reflink>]]. After calibration using information from both simulation and data [[<reflink idref="bib68" id="ref63">68</reflink>]], jets were required to have <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub><mo>></mo><mn>25</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mo stretchy="false">|</mo><mi>η</mi><mo stretchy="false">|</mo><mo><</mo><mn>2.5</mn></mrow></math> </ephtml> , and jets with <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub><mo><</mo><mn>60</mn></mrow></math> </ephtml> GeV and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mo stretchy="false">|</mo><mi>η</mi><mo stretchy="false">|</mo><mo><</mo><mn>2.4</mn></mrow></math> </ephtml> were subject to additional pileup rejection criteria using the multivariate jet-vertex tagger (JVT) [[<reflink idref="bib69" id="ref64">69</reflink>]]. To prevent double counting of electron energy deposits as jets, the closest jet to an electron candidate was removed if it was within <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi mathvariant="normal">Δ</mi><msub><mi>R</mi><mi>y</mi></msub><mo>=</mo><mn>0.2</mn></mrow></math> </ephtml> of the electron. Furthermore, to reduce the contribution of leptons from heavy-flavour hadron decays inside jets, leptons within <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi mathvariant="normal">Δ</mi><msub><mi>R</mi><mi>y</mi></msub><mo>=</mo><mn>0.4</mn></mrow></math> </ephtml> of selected jets were discarded, unless the lepton was a muon and the jet had fewer than three associated tracks, in which case the jet was discarded (thus avoiding an efficiency loss for high-energy muons undergoing significant energy loss in the calorimeters).</p> <p>Jets likely to contain <emph>b</emph>-hadrons were <emph>b</emph>-tagged using the MV2c10 algorithm [[<reflink idref="bib70" id="ref65">70</reflink>]], a multivariate discriminant making use of track impact parameters and reconstructed secondary vertices. A tagging working point corresponding to 70% efficiency for tagging <emph>b</emph>-quark jets from top quark decays in simulated <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> events was used, corresponding to rejection factors (i.e. the inverse of the mistag rates) of about 400 against light-quark and gluon jets and 12 against jets originating from charm quarks.</p> <p>Selected events were required to have exactly one electron and exactly one muon passing the requirements detailed above, with at least one of the leptons matched to a corresponding electron or muon trigger. Events where the electron and muon were separated in angle by <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mo stretchy="false">|</mo><mi mathvariant="normal">Δ</mi><mi>θ</mi><mo stretchy="false">|</mo><mo><</mo><mn>0.15</mn></mrow></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mo stretchy="false">|</mo><mi mathvariant="normal">Δ</mi><mi>ϕ</mi><mo stretchy="false">|</mo><mo><</mo><mn>0.15</mn></mrow></math> </ephtml> , or where at least one jet with <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub><mo>></mo><mn>20</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math> </ephtml> failed quality requirements [[<reflink idref="bib71" id="ref66">71</reflink>]], were rejected. Events with an opposite-sign <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>e</mi><mi>μ</mi></mrow></math> </ephtml> pair formed the main analysis sample, whilst events with a same-sign <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>e</mi><mi>μ</mi></mrow></math> </ephtml> pair were used in the estimation of background from misidentified leptons. Table 1 summarises the main selection requirements.</p> <p>Summary of the main object and event selection requirements</p> <p> <ephtml> <table frame="hsides" rules="groups"><thead><tr><th align="left"><p>Object</p></th><th align="left"><p>Identification</p></th><th align="left"><p>Selection</p></th></tr></thead><tbody><tr><td align="left"><p>Electrons</p></td><td align="left"><p>Tight likelihood</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msub><mi>E</mi><mi mathvariant="normal">T</mi></msub><mo>></mo><mn>20</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq206.gif" />, <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mo stretchy="false">|</mo><mi>η</mi><mo stretchy="false">|</mo><mo><</mo><mn>1.37</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq207.gif" /> or <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.52</mn><mo><</mo><mo stretchy="false">|</mo><mi>η</mi><mo stretchy="false">|</mo><mo><</mo><mn>2.47</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq208.gif" />, isolation</p></td></tr><tr><td align="left"><p>Muons</p></td><td align="left"><p>Medium</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub><mo>></mo><mn>20</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq209.gif" />, <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mo stretchy="false">|</mo><mi>η</mi><mo stretchy="false">|</mo><mo><</mo><mn>2.5</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq210.gif" />, isolation</p></td></tr><tr><td align="left"><p>Jets</p></td><td align="left"><p>Anti-<math xmlns="http://www.w3.org/1998/Math/MathML"><msub xmlns=""><mi>k</mi><mi>t</mi></msub></math><inline-graphic href="10052_2020_7907_Article_IEq211.gif" /><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>R</mi><mo>=</mo><mn>0.4</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq212.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub><mo>></mo><mn>25</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq213.gif" />, <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mo stretchy="false">|</mo><mi>η</mi><mo stretchy="false">|</mo><mo><</mo><mn>2.5</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq214.gif" />, <italic>b</italic>-tagging with MV2c10 at 70% efficiency</p></td></tr><tr><td align="left"><p>Event</p></td><td align="left" /><td align="left"><p>1 electron+1 muon with opposite sign, 1 or 2 <italic>b</italic>-tagged jets</p></td></tr></tbody></table> </ephtml> </p> <hd id="AN0144642803-5">Cross-section measurement</hd> <p>The same technique, employing the subsets of the opposite-sign <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>e</mi><mi>μ</mi></mrow></math> </ephtml> sample with exactly one and exactly two <emph>b</emph>-tagged jets, was used to measure both the inclusive <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> cross-section and the differential distributions. The measurements are introduced in the following two subsections, followed by a discussion of the background estimate in Sect. 4.3 and the validation of the differential measurements using studies based on simulation in Sect. 4.4.</p> <hd id="AN0144642803-6">Inclusive cross-sections</hd> <p>The inclusive <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> cross-section <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> was determined by counting the numbers of opposite-sign <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>e</mi><mi>μ</mi></mrow></math> </ephtml> events with exactly one ( <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>N</mi><mn>1</mn></msub></math> </ephtml> ) and exactly two ( <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>N</mi><mn>2</mn></msub></math> </ephtml> ) <emph>b</emph>-tagged jets. The two event counts satisfy the tagging equations:</p> <olist> <item> <ephtml> <math display="block" xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtable><mtr><mtd columnalign="right"><mrow><msub><mi>N</mi><mn>1</mn></msub><mo>=</mo></mrow></mtd><mtd columnalign="left"><mrow><mrow /><mi>L</mi><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub><mspace width="4pt" /><msub><mi>ϵ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msub><mn>2</mn><msub><mi>ϵ</mi><mi>b</mi></msub><mrow><mo stretchy="false">(</mo><mn>1</mn><mo>-</mo><msub><mi>C</mi><mi>b</mi></msub><msub><mi>ϵ</mi><mi>b</mi></msub><mo stretchy="false">)</mo></mrow><mo>+</mo><msubsup><mi>N</mi><mn>1</mn><mi mathvariant="normal">bkg</mi></msubsup><mo>,</mo></mrow></mtd></mtr><mtr><mtd columnalign="right"><mrow><mrow /><msub><mi>N</mi><mn>2</mn></msub><mo>=</mo></mrow></mtd><mtd columnalign="left"><mrow><mrow /><mi>L</mi><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub><mspace width="4pt" /><msub><mi>ϵ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msub><msub><mi>C</mi><mi>b</mi></msub><msubsup><mi>ϵ</mi><mrow><mi>b</mi></mrow><mn>2</mn></msubsup><mo>+</mo><msubsup><mi>N</mi><mn>2</mn><mi mathvariant="normal">bkg</mi></msubsup></mrow></mtd></mtr></mtable></mrow></math> </ephtml> </item> </olist> <p>Graph</p> <p>where <emph>L</emph> is the integrated luminosity of the sample, <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>ϵ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msub></math> </ephtml> the efficiency for a <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> event to pass the opposite-sign <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>e</mi><mi>μ</mi></mrow></math> </ephtml> selection, and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>C</mi><mi>b</mi></msub></math> </ephtml> is a tagging correlation coefficient close to unity. The combined probability for a jet from the quark <emph>q</emph> in the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mo stretchy="false">→</mo><mi>W</mi><mi>q</mi></mrow></math> </ephtml> decay to fall within the acceptance of the detector, be reconstructed as a jet with transverse momentum above the selection threshold, and be tagged as a <emph>b</emph>-jet, is denoted by <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>ϵ</mi><mi>b</mi></msub></math> </ephtml> . If the decays of the two top quarks and the reconstruction of the two associated <emph>b</emph>-tagged jets are completely independent, the probability <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>ϵ</mi><mrow><mi mathvariant="italic">bb</mi></mrow></msub></math> </ephtml> to reconstruct and tag both <emph>b</emph>-jets is given by <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>ϵ</mi><mrow><mi mathvariant="italic">bb</mi></mrow></msub><mo>=</mo><msubsup><mi>ϵ</mi><mrow><mi>b</mi></mrow><mn>2</mn></msubsup></mrow></math> </ephtml> . In practice, small correlations are present, due to kinematic correlations between the <emph>b</emph>-jets from the two top quarks, or the production of extra <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>b</mi><mover accent="true"><mrow><mi>b</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> or <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>c</mi><mover accent="true"><mrow><mi>c</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> pairs in the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> events. These effects are taken into account via the correlation coefficient <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>C</mi><mi>b</mi></msub><mo>=</mo><msub><mi>ϵ</mi><mrow><mi mathvariant="italic">bb</mi></mrow></msub><mo stretchy="false">/</mo><msubsup><mi>ϵ</mi><mrow><mi>b</mi></mrow><mn>2</mn></msubsup></mrow></math> </ephtml> , or equivalently <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>C</mi><mi>b</mi></msub><mo>=</mo><mn>4</mn><msubsup><mi>N</mi><mrow><mi>e</mi><mi>μ</mi></mrow><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msubsup><msubsup><mi>N</mi><mn>2</mn><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msubsup><mo stretchy="false">/</mo><msup><mrow><mo stretchy="false">(</mo><msubsup><mi>N</mi><mn>1</mn><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msubsup><mo>+</mo><mn>2</mn><msubsup><mi>N</mi><mn>2</mn><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msubsup><mo stretchy="false">)</mo></mrow><mn>2</mn></msup></mrow></math> </ephtml> , where <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>N</mi><mrow><mi>e</mi><mi>μ</mi></mrow><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msubsup></math> </ephtml> is the number of selected <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>e</mi><mi>μ</mi></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> events and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>N</mi><mn>1</mn><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msubsup></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>N</mi><mn>2</mn><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msubsup></math> </ephtml> are the numbers of such events with one and two <emph>b</emph>-tagged jets. In the baseline <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> simulation sample, <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>ϵ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msub><mo>≈</mo><mn>0.9</mn></mrow></math> </ephtml> %, including the branching ratio for a <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> pair to produce an <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>e</mi><mi>μ</mi></mrow></math> </ephtml> final state. The corresponding value of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>C</mi><mi>b</mi></msub></math> </ephtml> is <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mn>1.007</mn><mo>±</mo><mn>0.001</mn></mrow></math> </ephtml> (the uncertainty coming from the limited size of the simulation sample), indicating a small positive correlation between the reconstruction and <emph>b</emph>-tagging of the two quarks produced in the top quark decays. Background from sources other than <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> events with two prompt leptons also contributes to <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>N</mi><mn>1</mn></msub></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>N</mi><mn>2</mn></msub></math> </ephtml> and is given by the terms <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>N</mi><mn>1</mn><mi mathvariant="normal">bkg</mi></msubsup></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>N</mi><mn>2</mn><mi mathvariant="normal">bkg</mi></msubsup></math> </ephtml> , evaluated using a combination of simulation and data control samples as discussed in Sect. 4.3 below. The values of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>ϵ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msub></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>C</mi><mi>b</mi></msub></math> </ephtml> were taken from <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> event simulation, allowing the tagging equations (<reflink idref="bib1" id="ref67">1</reflink>) to be solved to determine <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>ϵ</mi><mi>b</mi></msub></math> </ephtml> .</p> <p>The selection efficiency <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>ϵ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msub></math> </ephtml> can be written as the product of two terms: <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>ϵ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msub><mo>=</mo><msub><mi>A</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msub><msub><mi>G</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msub></mrow></math> </ephtml> . The acceptance <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>A</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msub><mo>≈</mo><mn>1.7</mn></mrow></math> </ephtml> % represents the fraction of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> events which have a true opposite-sign <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>e</mi><mi>μ</mi></mrow></math> </ephtml> pair from <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mo stretchy="false">→</mo><mi>W</mi><mo stretchy="false">→</mo><mi>e</mi><mo stretchy="false">/</mo><mi>μ</mi></mrow></math> </ephtml> decays, with each lepton having <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub><mo>></mo><mn>20</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mo stretchy="false">|</mo><mi>η</mi><mo stretchy="false">|</mo><mo><</mo><mn>2.5</mn></mrow></math> </ephtml> . The contributions via leptonic <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mi>τ</mi></math> </ephtml> decays ( <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mo stretchy="false">→</mo><mi>W</mi><mo stretchy="false">→</mo><mi>τ</mi><mo stretchy="false">→</mo><mi>e</mi><mo stretchy="false">/</mo><mi>μ</mi></mrow></math> </ephtml> ) are included. The lepton four-momenta were taken after final-state radiation, and 'dressed' by including the four-momenta of any photons within a cone of size <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi mathvariant="normal">Δ</mi><mi>R</mi><mo>=</mo><mn>0.1</mn></mrow></math> </ephtml> around the lepton direction, excluding photons produced from hadron decays or interactions with the detector material. The reconstruction efficiency <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>G</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msub></math> </ephtml> represents the probability that the two leptons are reconstructed and pass all the identification and isolation requirements. A fiducial cross-section <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow><mi mathvariant="normal">fid</mi></msubsup></math> </ephtml> , for the production of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> events with an electron and a muon satisfying the requirements on <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mi>η</mi></math> </ephtml> , can then be defined as <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msubsup><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow><mi mathvariant="normal">fid</mi></msubsup><mo>=</mo><msub><mi>A</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msub><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></mrow></math> </ephtml> , and measured by replacing <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub><msub><mi>ϵ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msub></mrow></math> </ephtml> with <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msubsup><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow><mi mathvariant="normal">fid</mi></msubsup><msub><mi>G</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msub></mrow></math> </ephtml> in Eq. (<reflink idref="bib1" id="ref68">1</reflink>). The fiducial cross-section definition makes no requirements on the presence of jets, as the tagging formalism of Eq. (<reflink idref="bib1" id="ref69">1</reflink>) allows the number of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> events with no reconstructed and <emph>b</emph>-tagged jets to be inferred from the event counts <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>N</mi><mn>1</mn></msub></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>N</mi><mn>2</mn></msub></math> </ephtml> . Measurement of the fiducial cross-section avoids the systematic uncertainties associated with the evaluation of the acceptance, in particular estimation of the fraction of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo stretchy="false">→</mo><mi>e</mi><mi>μ</mi><mi>ν</mi><mover accent="true"><mrow><mi>ν</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mi>b</mi><mover accent="true"><mrow><mi>b</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> events where at least one lepton has <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub><mo><</mo><mn>20</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math> </ephtml> or <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mo stretchy="false">|</mo><mi>η</mi><mo stretchy="false">|</mo><mo>></mo><mn>2.5</mn></mrow></math> </ephtml> .</p> <p>A total of 40 680 data events passed the opposite-sign <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>e</mi><mi>μ</mi></mrow></math> </ephtml> selection in the 2015 data sample, and 358 664 events in the 2016 data sample. They were subdivided according to the number of <emph>b</emph>-tagged jets, irrespective of the number of untagged jets. The numbers of events with one and two <emph>b</emph>-tagged jets in each sample are shown in Table 2, together with the expected non- <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> contributions from <emph>Wt</emph> and dibosons evaluated from simulation, and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>Z</mi><mo stretchy="false">(</mo><mo stretchy="false">→</mo><mi>τ</mi><mi>τ</mi><mo stretchy="false">→</mo><mi>e</mi><mi>μ</mi><mo stretchy="false">)</mo></mrow></math> </ephtml> +jets and misidentified leptons evaluated using both data and simulation. The one <emph>b</emph>-tag sample is expected to be about 88% pure and the two <emph>b</emph>-tag sample 96% pure in <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> events, with the largest backgrounds in both samples coming from <emph>Wt</emph> production. The distribution of the number of <emph>b</emph>-tagged jets is shown for the 2015 and 2016 data samples together in Fig. 1a, and compared with the expectations from simulation, broken down into contributions from <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> events (modelled using the baseline Powheg + Pythia8 sample), and various background processes. The predictions using alternative <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> generator configurations (Powheg + Pythia8 with more or less parton-shower radiation, denoted by 'RadUp' and 'RadDn', and aMC@NLO + Pythia8) are also shown. All expected contributions are normalised to the integrated luminosity of the data sample using the cross-sections discussed in Sects. 1 and 2. The excess of data events over the prediction in the zero <emph>b</emph>-tagged jets sample (which is not used in the measurement) was also observed previously [[<reflink idref="bib7" id="ref70">7</reflink>], [<reflink idref="bib9" id="ref71">9</reflink>]] and is compatible with the expected uncertainties in modelling diboson and <emph>Z</emph>+jets production.</p> <p>Observed numbers of opposite-sign <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>e</mi><mi>μ</mi></mrow></math> </ephtml> events with one ( <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>N</mi><mn>1</mn></msub></math> </ephtml> ) and two ( <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>N</mi><mn>2</mn></msub></math> </ephtml> ) <emph>b</emph>-tagged jets in 2015 and 2016 data, together with the estimates of backgrounds and associated uncertainties described in Sect. 5. Uncertainties shown as zero are less than 0.5 events</p> <p> <ephtml> <table frame="hsides" rules="groups"><thead><tr><th align="left"><p>Sample</p></th><th align="left" colspan="2"><p>2015</p></th><th align="left" colspan="2"><p>2016</p></th></tr><tr><th align="left"><p>Event counts</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><msub xmlns=""><mi>N</mi><mn>1</mn></msub></math><inline-graphic href="10052_2020_7907_Article_IEq290.gif" /></p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><msub xmlns=""><mi>N</mi><mn>2</mn></msub></math><inline-graphic href="10052_2020_7907_Article_IEq291.gif" /></p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><msub xmlns=""><mi>N</mi><mn>1</mn></msub></math><inline-graphic href="10052_2020_7907_Article_IEq292.gif" /></p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><msub xmlns=""><mi>N</mi><mn>2</mn></msub></math><inline-graphic href="10052_2020_7907_Article_IEq293.gif" /></p></th></tr><tr><th align="left"><p>Data</p></th><th align="left"><p>14239</p></th><th align="left"><p>8351</p></th><th align="left"><p>133977</p></th><th align="left"><p>75853</p></th></tr></thead><tbody><tr><td align="left"><p><italic>Wt</italic> single top</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1329</mn><mo>±</mo><mn>92</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq294.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>261</mn><mo>±</mo><mn>86</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq295.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>12490</mn><mo>±</mo><mn>870</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq296.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2430</mn><mo>±</mo><mn>810</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq297.gif" /></p></td></tr><tr><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>Z</mi><mo stretchy="false">(</mo><mo stretchy="false">→</mo><mi>τ</mi><mi>τ</mi><mo stretchy="false">→</mo><mi>e</mi><mi>μ</mi><mo stretchy="false">)</mo><mo>+</mo><mtext>jets</mtext></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq298.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>123</mn><mo>±</mo><mn>15</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq299.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>7</mn><mo>±</mo><mn>2</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq300.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>910</mn><mo>±</mo><mn>110</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq301.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>37</mn><mo>±</mo><mn>9</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq302.gif" /></p></td></tr><tr><td align="left"><p>Diboson</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>42</mn><mo>±</mo><mn>5</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq303.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1</mn><mo>±</mo><mn>0</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq304.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>481</mn><mo>±</mo><mn>58</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq305.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>21</mn><mo>±</mo><mn>7</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq306.gif" /></p></td></tr><tr><td align="left"><p>Misidentified leptons</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>164</mn><mo>±</mo><mn>54</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq307.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>58</mn><mo>±</mo><mn>37</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq308.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1720</mn><mo>±</mo><mn>520</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq309.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>670</mn><mo>±</mo><mn>390</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq310.gif" /></p></td></tr><tr><td align="left"><p>Total background</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1660</mn><mo>±</mo><mn>110</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq311.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>327</mn><mo>±</mo><mn>94</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq312.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>15600</mn><mo>±</mo><mn>1000</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq313.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3160</mn><mo>±</mo><mn>890</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq314.gif" /></p></td></tr></tbody></table> </ephtml> </p> <p>Graph: Fig. 1 Distributions of a the number of b-tagged jets in selected opposite-sign eμ events; and b the pT of b-tagged jets, c the pT of the electron, d the |η| of the electron, e the pT of the muon and f the |η| of the muon, in events with an opposite-sign eμ pair and at least one b-tagged jet. The reconstruction-level data are compared with the expectation from simulation, broken down into contributions from tt¯ (Powheg + Pythia8), Wt, Z+jets, dibosons, and events with misidentified electrons or muons. The simulation prediction is normalised to the same integrated luminosity as the data in a and to the same number of entries as the data in b–f. The lower parts of the figure show the ratios of simulation to data, using various tt¯ signal samples and with the cyan shaded band indicating the statistical uncertainty. The last bin includes the overflow in panels b, c and e</p> <p>Figure 1b–f show distributions of the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> of the <emph>b</emph>-tagged jets, and the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mo stretchy="false">|</mo><mi>η</mi><mo stretchy="false">|</mo></mrow></math> </ephtml> of the electron and muon, in opposite-sign <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>e</mi><mi>μ</mi></mrow></math> </ephtml> events with at least one <emph>b</emph>-tagged jet, a sample which is dominated by <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> events. The total simulation prediction is normalised to the same number of events as the data to facilitate shape comparisons. The <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mo stretchy="false">|</mo><mi>η</mi><mo stretchy="false">|</mo></mrow></math> </ephtml> distributions for electrons and muons reflect the differences in acceptance and efficiency, in particular the reduction in electron acceptance across the calorimeter transition region, and the reduced acceptance for muons around <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mo stretchy="false">|</mo><mi>η</mi><mo stretchy="false">|</mo><mo>≈</mo><mn>0</mn></mrow></math> </ephtml> . In general, the simulation predictions give a good description of the data, although the baseline Powheg + Pythia8 simulation predicts a significantly harder lepton <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> distribution than seen in data.</p> <p>The inclusive cross-section was determined separately from the 2015 and 2016 datasets, and the results were combined, taking into account correlations in the systematic uncertainties. As the systematic uncertainties are much larger than the statistical uncertainties, and not fully correlated between the two samples (true in particular for the uncertainty in the integrated luminosity), this procedure gives a smaller overall uncertainty than treating the 2015–2016 data as a single sample. The selection efficiency <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>ϵ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msub></math> </ephtml> is about 10% lower in the 2016 data compared to the 2015 data, due to the harsher pileup conditions and higher- <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> trigger thresholds.</p> <hd id="AN0144642803-7">Differential cross-sections</hd> <p>The differential cross-sections as functions of the lepton and dilepton variables defined in Sect. 1 were measured using an extension of Eq. (<reflink idref="bib1" id="ref72">1</reflink>), by counting the number of leptons or events with one ( <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>N</mi><mn>1</mn><mi>i</mi></msubsup></math> </ephtml> ) or two ( <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>N</mi><mn>2</mn><mi>i</mi></msubsup></math> </ephtml> ) <emph>b</emph>-tagged jets where the lepton(s) falls in bin <emph>i</emph> of a differential distribution at reconstruction level. For the single-lepton distributions <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>ℓ</mi></msubsup></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>η</mi><mi>ℓ</mi></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> , there are two counts per event, in the two bins corresponding to the electron and muon. For the dilepton distributions, each event contributes a single count corresponding to the bin in which the appropriate dilepton variable falls. For each bin of each differential distribution, these counts satisfy the tagging equations:</p> <p>2 <ephtml> <math display="block" xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtable><mtr><mtd columnalign="right"><mrow><msubsup><mi>N</mi><mn>1</mn><mi>i</mi></msubsup><mo>=</mo></mrow></mtd><mtd columnalign="left"><mrow><mrow /><mi>L</mi><msubsup><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow><mi>i</mi></msubsup><mspace width="4pt" /><msubsup><mi>G</mi><mrow><mi>e</mi><mi>μ</mi></mrow><mi>i</mi></msubsup><mn>2</mn><msubsup><mi>ϵ</mi><mi>b</mi><mi>i</mi></msubsup><mrow><mo stretchy="false">(</mo><mn>1</mn><mo>-</mo><msubsup><mi>C</mi><mi>b</mi><mi>i</mi></msubsup><msubsup><mi>ϵ</mi><mi>b</mi><mi>i</mi></msubsup><mo stretchy="false">)</mo></mrow><mo>+</mo><msubsup><mi>N</mi><mn>1</mn><mrow><mi>i</mi><mo>,</mo><mi mathvariant="normal">bkg</mi></mrow></msubsup><mo>,</mo></mrow></mtd></mtr><mtr><mtd columnalign="right"><mrow><mrow /><msubsup><mi>N</mi><mn>2</mn><mi>i</mi></msubsup><mo>=</mo></mrow></mtd><mtd columnalign="left"><mrow><mrow /><mi>L</mi><msubsup><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow><mi>i</mi></msubsup><mspace width="4pt" /><msubsup><mi>G</mi><mrow><mi>e</mi><mi>μ</mi></mrow><mi>i</mi></msubsup><msubsup><mi>C</mi><mi>b</mi><mi>i</mi></msubsup><msup><mrow><mo stretchy="false">(</mo><msubsup><mi>ϵ</mi><mi>b</mi><mi>i</mi></msubsup><mo stretchy="false">)</mo></mrow><mn>2</mn></msup><mo>+</mo><msubsup><mi>N</mi><mn>2</mn><mrow><mi>i</mi><mo>,</mo><mi mathvariant="normal">bkg</mi></mrow></msubsup><mo>,</mo></mrow></mtd></mtr></mtable></mrow></math> </ephtml></p> <p>Graph</p> <p>where <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow><mi>i</mi></msubsup></math> </ephtml> is the absolute fiducial differential cross-section in bin <emph>i</emph>. The reconstruction efficiency <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>G</mi><mrow><mi>e</mi><mi>μ</mi></mrow><mi>i</mi></msubsup></math> </ephtml> represents the ratio of the number of reconstructed <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>e</mi><mi>μ</mi></mrow></math> </ephtml> events (or leptons for <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>ℓ</mi></msubsup></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>η</mi><mi>ℓ</mi></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> ) in bin <emph>i</emph> defined using the reconstructed lepton(s), to the number of true <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>e</mi><mi>μ</mi></mrow></math> </ephtml> events (or leptons) in the same bin <emph>i</emph> at particle level, evaluated using <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> simulation. The true electron and muon were required to have <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub><mo>></mo><mn>20</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mo stretchy="false">|</mo><mi>η</mi><mo stretchy="false">|</mo><mo><</mo><mn>2.5</mn></mrow></math> </ephtml> , but no requirements were made on reconstructed or particle-level jets. The efficiency <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>G</mi><mrow><mi>e</mi><mi>μ</mi></mrow><mi>i</mi></msubsup></math> </ephtml> corrects for both the lepton reconstruction efficiency and the effects of event migration, where events in bin <emph>j</emph> at particle level appear in a different bin <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>i</mi><mo>≠</mo><mi>j</mi></mrow></math> </ephtml> at reconstruction level. The integral of any dilepton differential cross-section is equal to the fiducial cross-section <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow><mi mathvariant="normal">fid</mi></msubsup></math> </ephtml> defined in Sect. 4.1, and the integrals of the single-lepton <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>ℓ</mi></msubsup></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>η</mi><mi>ℓ</mi></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> distributions are equal to <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mn>2</mn><msubsup><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow><mi mathvariant="normal">fid</mi></msubsup></mrow></math> </ephtml> . The correlation coefficient <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>C</mi><mi>b</mi><mi>i</mi></msubsup></math> </ephtml> depends on the event counts in bin <emph>i</emph> analogously to the inclusive <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>C</mi><mi>b</mi></msub></math> </ephtml> appearing in Eq. (<reflink idref="bib1" id="ref73">1</reflink>). The values of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>G</mi><mrow><mi>e</mi><mi>μ</mi></mrow><mi>i</mi></msubsup></math> </ephtml> were taken from <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> simulation, and are generally around 0.5–0.6. The corresponding values of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>C</mi><mi>b</mi><mi>i</mi></msubsup></math> </ephtml> are always within 1–2% of unity, even at the edges of the differential distribution. The background term <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>N</mi><mn>1</mn><mrow><mi>i</mi><mo>,</mo><mi mathvariant="normal">bkg</mi></mrow></msubsup></math> </ephtml> varies from 11% to 23% of the total event count <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>N</mi><mn>1</mn><mi>i</mi></msubsup></math> </ephtml> in each bin, and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>N</mi><mn>2</mn><mrow><mi>i</mi><mo>,</mo><mi mathvariant="normal">bkg</mi></mrow></msubsup></math> </ephtml> varies from 3% to 14% of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>N</mi><mn>2</mn><mi>i</mi></msubsup></math> </ephtml> . They were determined from simulation and data control samples, allowing the tagging equations (<reflink idref="bib2" id="ref74">2</reflink>) to be solved to give the absolute fiducial differential cross-sections <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow><mi>i</mi></msubsup></math> </ephtml> and associated <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>ϵ</mi><mi>b</mi><mi>i</mi></msubsup></math> </ephtml> values for each bin <emph>i</emph> of each differential distribution.</p> <p>The bin ranges for each differential distribution were based on those used at <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>8</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> [[<reflink idref="bib29" id="ref75">29</reflink>]], adding an additional bin for 20–25 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> in the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>ℓ</mi></msubsup></math> </ephtml> distribution and extending the lowest bin down to 40 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> for <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>e</mi></msubsup><mo>+</mo><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>μ</mi></msubsup></mrow></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msup><mi>E</mi><mi>e</mi></msup><mo>+</mo><msup><mi>E</mi><mi>μ</mi></msup></mrow></math> </ephtml> to accommodate the reduced minimum lepton <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> requirement of 20 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> . The number and sizes of bins were chosen according to the experimental resolution in order to keep the bin purities (i.e the fractions of events reconstructed in bin <emph>i</emph> that originate from bin <emph>i</emph> at particle level) above about 0.9, and to keep a maximum of around ten bins for the angular distributions ( <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>η</mi><mi>ℓ</mi></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> , <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>y</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi mathvariant="normal">Δ</mi><msup><mi>ϕ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math> </ephtml> ). The variations in the angular distributions predicted by different <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> models do not motivate a finer binning, even though the experimental resolution would allow it. The chosen bin ranges can be seen in Tables 15, 16, 17, 18 in the Appendix. The last bin of the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>ℓ</mi></msubsup></math> </ephtml> , <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mrow><mi>e</mi><mi>μ</mi></mrow></msubsup></math> </ephtml> , <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></math> </ephtml> , <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>e</mi></msubsup><mo>+</mo><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>μ</mi></msubsup></mrow></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msup><mi>E</mi><mi>e</mi></msup><mo>+</mo><msup><mi>E</mi><mi>μ</mi></msup></mrow></math> </ephtml> distributions includes overflow events falling above the last bin boundary.</p> <p>The normalised fiducial differential cross-sections <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>ς</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow><mi>i</mi></msubsup></math> </ephtml> were calculated from the absolute cross-sections <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow><mi>i</mi></msubsup></math> </ephtml> as follows:</p> <p>3 <ephtml> <math display="block" xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtable><mtr><mtd columnalign="right"><mrow><msubsup><mi>ς</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow><mi>i</mi></msubsup><mo>=</mo><mfrac><msubsup><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow><mi>i</mi></msubsup><mrow><msub><mi mathvariant="normal">Σ</mi><mi>j</mi></msub><mspace width="4pt" /><msubsup><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow><mi>j</mi></msubsup></mrow></mfrac><mo>=</mo><mfrac><msubsup><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow><mi>i</mi></msubsup><msubsup><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow><mi mathvariant="normal">fid</mi></msubsup></mfrac><mo>,</mo></mrow></mtd></mtr></mtable></mrow></math> </ephtml></p> <p>Graph</p> <p>where <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow><mi mathvariant="normal">fid</mi></msubsup></math> </ephtml> is the cross-section summed over all bins of the fiducial region, equal to the fiducial cross-section defined in Sect. 4.1, or twice that in the case of the single-lepton distributions. The <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>ς</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow><mi>i</mi></msubsup></math> </ephtml> values were then divided by the bin widths <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>W</mi><mi>i</mi></msub></math> </ephtml> , to produce the cross-sections differential in the variable <emph>x</emph> ( <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>x</mi><mo>=</mo><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>ℓ</mi></msubsup></mrow></math> </ephtml> , <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>η</mi><mi>ℓ</mi></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> , etc.):</p> <p>4 <ephtml> <math display="block" xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtable><mtr><mtd columnalign="right"><mrow><mfrac><mn>1</mn><mi>σ</mi></mfrac><msub><mfenced close=")" open="(" separators=""><mfrac><mrow><mi mathvariant="normal">d</mi><mi>σ</mi></mrow><mrow><mi mathvariant="normal">d</mi><mi>x</mi></mrow></mfrac></mfenced><mi>i</mi></msub><mo>=</mo><mfrac><msubsup><mi>ς</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow><mi>i</mi></msubsup><msub><mi>W</mi><mi>i</mi></msub></mfrac><mo>.</mo></mrow></mtd></mtr></mtable></mrow></math> </ephtml></p> <p>Graph</p> <p>The normalised differential cross-sections are correlated between bins because of the normalisation condition in Eq. (<reflink idref="bib3" id="ref76">3</reflink>). The absolute dilepton differential cross-sections are not statistically correlated between bins, but kinematic correlations between the electron and muon within one event introduce small correlations within the absolute single-lepton <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>ℓ</mi></msubsup></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>η</mi><mi>ℓ</mi></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> distributions.</p> <p>The larger number of selected <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> events compared to the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>8</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> analysis allows double-differential cross-sections to be measured, i.e. distributions that are functions of two variables. Three such distributions were measured, with <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>η</mi><mi>ℓ</mi></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> , <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>y</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> or <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi mathvariant="normal">Δ</mi><msup><mi>ϕ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math> </ephtml> as the first variable, and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></math> </ephtml> as the second variable, effectively measuring the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>η</mi><mi>ℓ</mi></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> , <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>y</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi mathvariant="normal">Δ</mi><msup><mi>ϕ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math> </ephtml> distributions in four bins of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></math> </ephtml> , chosen to be <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mo><</mo><mn>80</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math> </ephtml> , <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mn>80</mn><mo><</mo><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mo><</mo><mn>120</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math> </ephtml> , <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mn>120</mn><mo><</mo><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mo><</mo><mn>200</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mo>></mo><mn>200</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math> </ephtml> . The excellent resolution in <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>η</mi><mi>ℓ</mi></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> , <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>y</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi mathvariant="normal">Δ</mi><msup><mi>ϕ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math> </ephtml> results in migration effects being significant only between <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></math> </ephtml> bins. The formalism of Eq. (<reflink idref="bib2" id="ref77">2</reflink>) was used, with the index <emph>i</emph> running over the two-dimensional grid of bins in both variables. The normalised double-differential cross-sections were calculated with the sum in the denominator of Eq. (<reflink idref="bib3" id="ref78">3</reflink>) running over all bins, making the integral of the normalised double-differential cross-section equal to unity over the entire fiducial region, rather than normalising e.g. the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>η</mi><mi>ℓ</mi></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> distribution to unity in each <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></math> </ephtml> bin separately.</p> <p>The measured differential cross-sections include contributions where one or both leptons are produced via leptonic decays of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mi>τ</mi></math> </ephtml> -leptons ( <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mo stretchy="false">→</mo><mi>W</mi><mo stretchy="false">→</mo><mi>τ</mi><mo stretchy="false">→</mo><mi>e</mi><mo stretchy="false">/</mo><mi>μ</mi></mrow></math> </ephtml> ). To enable comparisons with theoretical predictions which only include direct <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mo stretchy="false">→</mo><mi>W</mi><mo stretchy="false">→</mo><mi>e</mi><mo stretchy="false">/</mo><mi>μ</mi></mrow></math> </ephtml> decays, a second set of cross-section results was derived with a bin-by-bin multiplicative correction <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>f</mi><mrow><mi mathvariant="normal">no</mi><mo>-</mo><mi>τ</mi></mrow><mi>i</mi></msubsup></math> </ephtml> to remove the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mi>τ</mi></math> </ephtml> contributions:</p> <p>5 <ephtml> <math display="block" xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtable><mtr><mtd columnalign="right"><mrow><msubsup><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow><mi>i</mi></msubsup><mspace width="0.166667em" /><mrow><mo stretchy="false">(</mo><mspace width="0.333333em" /><mtext>no-</mtext><mspace width="0.333333em" /><mi>τ</mi><mo stretchy="false">)</mo></mrow><mo>=</mo><msubsup><mi>f</mi><mrow><mi mathvariant="normal">no</mi><mo>-</mo><mi>τ</mi></mrow><mi>i</mi></msubsup><msubsup><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow><mi>i</mi></msubsup><mo>,</mo></mrow></mtd></mtr></mtable></mrow></math> </ephtml></p> <p>Graph</p> <p>and similarly for the normalised cross-sections <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msubsup><mi>ς</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow><mi>i</mi></msubsup><mspace width="0.166667em" /><mrow><mo stretchy="false">(</mo><mspace width="0.333333em" /><mtext>no-</mtext><mspace width="0.333333em" /><mi>τ</mi><mo stretchy="false">)</mo></mrow></mrow></math> </ephtml> . The corrections <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>f</mi><mrow><mi mathvariant="normal">no</mi><mo>-</mo><mi>τ</mi></mrow><mi>i</mi></msubsup></math> </ephtml> were evaluated from the baseline Powheg + Pythia8 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> simulation as the fractions of leptons or events in each particle-level bin which do not involve <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mi>τ</mi></math> </ephtml> -lepton decays. They are typically in the range 0.8–0.9, the smaller values occurring in bins with a large contribution of low- <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> leptons where the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mi>τ</mi></math> </ephtml> contributions are largest.</p> <p>Since the uncertainties in most of the differential cross-section bins are dominated by the data statistical uncertainties, and the luminosity uncertainty largely cancels out in the normalised differential cross-sections, the 2015–2016 data were treated as a single sample in the differential analysis. The varying lepton trigger thresholds and offline identification efficiencies were taken into account by calculating <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>G</mi><mrow><mi>e</mi><mi>μ</mi></mrow><mi>i</mi></msubsup></math> </ephtml> from an appropriately weighted mixture of simulated events. Figure 2 shows the reconstructed dilepton distributions for events with at least one <emph>b</emph>-tagged jet, comparing data with predictions using various <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> generator configurations. As in Figure 1b–f, the predictions generally describe the data well, although in some regions there are significant differences between the data and all predictions, which are discussed further in Sect. 7.2 below.</p> <p>Graph: Fig. 2 Distributions of a the dilepton pTeμ, b invariant mass meμ, c rapidity |yeμ|, d azimuthal angle difference Δϕeμ, e lepton pT sum pTe+pTμ and f lepton energy sum Ee+Eμ, in events with an opposite-sign eμ pair and at least one b-tagged jet. The reconstruction-level data are compared with the expectation from simulation, broken down into contributions from tt¯ (Powheg + Pythia8), Wt, Z+jets, dibosons, and events with misidentified electrons or muons, normalised to the same number of entries as the data. The lower parts of the figure show the ratios of simulation to data, using various tt¯ signal samples and with the cyan shaded band indicating the statistical uncertainty. The last bin includes the overflow in panels a, b, e and f</p> <hd id="AN0144642803-8">Background estimates</hd> <p>The dominant background from <emph>Wt</emph> production, and the smaller contribution from diboson events (dominated by <emph>WW</emph> production) were evaluated from simulation, using the samples detailed in Sect. 2. The production of a <emph>Z</emph> boson accompanied by heavy-flavour jets is subject to large theoretical uncertainties, so the background contributions in the one and two <emph>b</emph>-tag samples predicted by Sherpa (normalised to the inclusive <emph>Z</emph> cross-section predictions from FEWZ [[<reflink idref="bib72" id="ref79">72</reflink>]]) were further scaled by factors of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mn>1.10</mn><mo>±</mo><mn>0.12</mn></mrow></math> </ephtml> (one <emph>b</emph>-tag) and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mn>1.20</mn><mo>±</mo><mn>0.12</mn></mrow></math> </ephtml> (two <emph>b</emph>-tags) obtained from data. These scale factors were derived from the ratio of data to simulation event yields for <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>Z</mi><mo stretchy="false">→</mo><mi>e</mi><mi>e</mi><mo stretchy="false">/</mo><mi>μ</mi><mi>μ</mi></mrow></math> </ephtml> accompanied by one or by two <emph>b</emph>-tagged jets. The <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>Z</mi><mo stretchy="false">→</mo><mi>e</mi><mi>e</mi><mo stretchy="false">/</mo><mi>μ</mi><mi>μ</mi></mrow></math> </ephtml> yields were obtained by requiring two opposite-sign electrons or muons passing the selections detailed in Sect. 3, and performing a template fit to the dilepton invariant mass distribution in the range <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mn>30</mn><mo><</mo><msub><mi>m</mi><mrow><mi>ℓ</mi><mi>ℓ</mi></mrow></msub><mo><</mo><mn>150</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math> </ephtml> in order to subtract the contributions from <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> events and misidentified leptons. The uncertainties are dominated by variations in the scale factors as functions of <emph>Z</emph> boson <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> . Further uncertainties of 5% in the one <emph>b</emph>-tag sample and 23% in the two <emph>b</emph>-tag sample were assigned from the change in the final background prediction when replacing the Sherpa sample with one generated using MadGraph [[<reflink idref="bib73" id="ref80">73</reflink>]] interfaced to Pythia8, including re-evaluation of the scale factors. Similar procedures were used to evaluate the uncertainty in the <emph>Z</emph>+jets background prediction in every bin of the differential distributions, including a comparison of the per-bin predictions from Sherpa and Madgraph after normalising each sample to data in the inclusive <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>Z</mi><mo stretchy="false">→</mo><mi>e</mi><mi>e</mi><mo stretchy="false">/</mo><mi>μ</mi><mi>μ</mi></mrow></math> </ephtml> control regions.</p> <p>The background from events with one real and one misidentified lepton was evaluated with the help of the same-sign <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>e</mi><mi>μ</mi></mrow></math> </ephtml> control sample. For the inclusive cross-section analysis, the contributions <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>N</mi><mi>j</mi><mrow><mi mathvariant="normal">mis</mi><mo>-</mo><mi mathvariant="normal">id</mi></mrow></msubsup></math> </ephtml> to the total numbers <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>N</mi><mi>j</mi></msub></math> </ephtml> of opposite-sign <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>e</mi><mi>μ</mi></mrow></math> </ephtml> events with <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>j</mi><mo>=</mo><mn>1</mn><mo>,</mo><mn>2</mn></mrow></math> </ephtml><emph>b</emph>-tagged jets are given by:</p> <p>6 <ephtml> <math display="block" xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtable><mtr><mtd columnalign="right"><mrow><msubsup><mi>N</mi><mi>j</mi><mrow><mi mathvariant="normal">mis</mi><mo>-</mo><mi mathvariant="normal">id</mi></mrow></msubsup><mo>=</mo></mrow></mtd><mtd columnalign="left"><mrow><mrow /><msub><mi>R</mi><mi>j</mi></msub><mfenced close=")" open="(" separators=""><msubsup><mi>N</mi><mi>j</mi><mrow><mi mathvariant="normal">data</mi><mo>,</mo><mi mathvariant="normal">SS</mi></mrow></msubsup><mo>-</mo><msubsup><mi>N</mi><mi>j</mi><mrow><mi mathvariant="normal">sim</mi><mo>,</mo><mi mathvariant="normal">prompt</mi><mo>,</mo><mi mathvariant="normal">SS</mi></mrow></msubsup></mfenced><mo>,</mo></mrow></mtd></mtr><mtr><mtd columnalign="right"><mrow><mrow /><msub><mi>R</mi><mi>j</mi></msub><mo>=</mo></mrow></mtd><mtd columnalign="left"><mrow><mrow /><mfrac><msubsup><mi>N</mi><mi>j</mi><mrow><mi mathvariant="normal">sim</mi><mo>,</mo><mi mathvariant="normal">mis</mi><mo>-</mo><mi mathvariant="normal">id</mi><mo>,</mo><mi mathvariant="normal">OS</mi></mrow></msubsup><msubsup><mi>N</mi><mi>j</mi><mrow><mi mathvariant="normal">sim</mi><mo>,</mo><mi mathvariant="normal">mis</mi><mo>-</mo><mi mathvariant="normal">id</mi><mo>,</mo><mi mathvariant="normal">SS</mi></mrow></msubsup></mfrac><mo>,</mo></mrow></mtd></mtr></mtable></mrow></math> </ephtml></p> <p>Graph</p> <p>where <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>N</mi><mi>j</mi><mrow><mi mathvariant="normal">data</mi><mo>,</mo><mi mathvariant="normal">SS</mi></mrow></msubsup></math> </ephtml> is the number of observed same-sign events, <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>N</mi><mi>j</mi><mrow><mi mathvariant="normal">sim</mi><mo>,</mo><mi mathvariant="normal">prompt</mi><mo>,</mo><mi mathvariant="normal">SS</mi></mrow></msubsup></math> </ephtml> is the number of same-sign events with two prompt leptons estimated from simulation, and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>R</mi><mi>j</mi></msub></math> </ephtml> is the ratio in simulation of the number of opposite-sign ( <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>N</mi><mi>j</mi><mrow><mi mathvariant="normal">sim</mi><mo>,</mo><mi mathvariant="normal">mis</mi><mo>-</mo><mi mathvariant="normal">id</mi><mo>,</mo><mi mathvariant="normal">OS</mi></mrow></msubsup></math> </ephtml> ) to same-sign ( <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>N</mi><mi>j</mi><mrow><mi mathvariant="normal">sim</mi><mo>,</mo><mi mathvariant="normal">mis</mi><mo>-</mo><mi mathvariant="normal">id</mi><mo>,</mo><mi mathvariant="normal">SS</mi></mrow></msubsup></math> </ephtml> ) events with misidentified leptons, all with <emph>j</emph><emph>b</emph>-tagged jets. This formalism relies on simulation to predict the ratio of opposite- to same-sign misidentified-lepton events, and the prompt same-sign contribution, but not the absolute number of misidentified-lepton events <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>N</mi><mi>j</mi><mrow><mi mathvariant="normal">mis</mi><mo>-</mo><mi mathvariant="normal">id</mi></mrow></msubsup></math> </ephtml> , which is calculated using the same-sign event counts in data. The same formalism in bins <emph>i</emph> of lepton differential variables was used to estimate the misidentified-lepton background contributions to <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>N</mi><mn>1</mn><mrow><mi>i</mi><mo>,</mo><mi mathvariant="normal">bkg</mi></mrow></msubsup></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>N</mi><mn>2</mn><mrow><mi>i</mi><mo>,</mo><mi mathvariant="normal">bkg</mi></mrow></msubsup></math> </ephtml> in each bin of the differential cross-section analysis.</p> <p>Table 3 shows the estimates from simulation of misidentified-lepton contributions to the opposite- and same-sign event counts in the inclusive cross-section analysis, separately for the 2015 and 2016 selections. The prompt contributions (corresponding to <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>N</mi><mi>j</mi><mrow><mi mathvariant="normal">sim</mi><mo>,</mo><mi mathvariant="normal">prompt</mi><mo>,</mo><mi mathvariant="normal">SS</mi></mrow></msubsup></math> </ephtml> in Eq. (<reflink idref="bib6" id="ref81">6</reflink>)) are about 25% of the one <emph>b</emph>-tag and 35% of the two <emph>b</emph>-tag same-sign samples. They include 'wrong-sign' contributions, dominated by dilepton <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> events where the electron charge sign has been misidentified, and 'right-sign' contributions, with two genuine same-sign prompt leptons, from <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo>+</mo><mi>V</mi></mrow></math> </ephtml> events ( <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>V</mi><mo>=</mo><mi>W</mi></mrow></math> </ephtml> , <emph>Z</emph> or <emph>H</emph>), <emph>WZ</emph>, <emph>ZZ</emph> or same-sign <emph>WW</emph> production. The misidentified-lepton contributions are dominated by electrons from photon conversions, shown separately for events where the photon was radiated from a prompt electron in a <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> dilepton event, or came from some other background source. These contributions are followed by electrons or muons from the semileptonic decays of heavy-flavour hadrons (e.g <emph>b</emph>-hadrons produced from the top quark decays, or charm hadrons produced from hadronic <emph>W</emph> decays in single-lepton <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> events), and other sources, such as misidentified hadrons or decays in flight of pions and kaons. Within each category and <emph>b</emph>-jet multiplicity, the numbers of opposite- and same-sign events are comparable, but with up to a factor two more opposite- than same-sign events in the major categories, and larger variations for the small contributions labelled 'Other'. The reasons for this behaviour are complex, depending e.g. on details of the electron reconstruction, or on charge correlations between the decay products of the two top quarks.</p> <p>The composition of the same-sign samples is also illustrated in Fig. 3, which shows electron and muon <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mo stretchy="false">|</mo><mi>η</mi><mo stretchy="false">|</mo></mrow></math> </ephtml> distributions in same-sign data events with at least one <emph>b</emph>-tagged jet, and the corresponding simulation predictions, broken down into prompt leptons (combining the right- and wrong-sign categories of Table 3) and various misidentified-lepton categories (again combining 'other' electrons and muons into a single category). Table 3 shows that the simulation reproduces the observed numbers of same-sign events well, and the distributions shown in Fig. 3 demonstrate that it also reproduces the general features of the lepton kinematic distributions, the largest differences in individual bins being around 20%. These studies validate the overall modelling of misidentified leptons by the simulation, even though the background estimates determined via Eq. (<reflink idref="bib6" id="ref82">6</reflink>) do not rely on the simulation providing an accurate estimate of the absolute rates of such events. Additional studies were performed using same-sign control samples with relaxed electron or muon isolation criteria (increasing the relative contribution of heavy-flavour decays), and changing the lepton selection to <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub><mo>></mo><mn>40</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math> </ephtml> (enhancing the fraction of photon conversions), and a similar level of agreement was seen both in rates and distribution shapes.</p> <p>Breakdown of estimated misidentified-lepton contributions in simulation to the one (1<emph>b</emph>) and two (2<emph>b</emph>) <emph>b</emph>-tag opposite- and same-sign (OS and SS) <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>e</mi><mi>μ</mi></mrow></math> </ephtml> event samples from 2015 and 2016 separately. The various misidentified-lepton categories are described in Sect. 4.3, and the contributions labelled 'Other' include all sources other than photon conversions and heavy-flavour decays. For the same-sign samples, the estimated contributions of wrong-sign (where the electron charge sign is misidentified) and right-sign prompt lepton events are also shown, and the total expectations are compared with the data. The uncertainties are due to the limited size of the simulated samples, and values or uncertainties shown as zero are less than 0.5 events</p> <p> <ephtml> <table frame="hsides" rules="groups"><thead><tr><th align="left" rowspan="2"><p>Component</p></th><th align="left" colspan="4"><p>2015</p></th><th align="left" colspan="4"><p>2016</p></th></tr><tr><th align="left"><p>OS 1<italic>b</italic></p></th><th align="left"><p>SS 1<italic>b</italic></p></th><th align="left"><p>OS 2<italic>b</italic></p></th><th align="left"><p>SS 2<italic>b</italic></p></th><th align="left"><p>OS 1<italic>b</italic></p></th><th align="left"><p>SS 1<italic>b</italic></p></th><th align="left"><p>OS 2<italic>b</italic></p></th><th align="left"><p>SS 2<italic>b</italic></p></th></tr></thead><tbody><tr><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>t</mi><mo stretchy="false">→</mo><mi>e</mi><mo stretchy="false">→</mo><mi>γ</mi></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq466.gif" /> conversion <italic>e</italic></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>59</mn><mo>±</mo><mn>5</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq467.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>41</mn><mo>±</mo><mn>4</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq468.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>33</mn><mo>±</mo><mn>3</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq469.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>21</mn><mo>±</mo><mn>3</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq470.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>594</mn><mo>±</mo><mn>15</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq471.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>360</mn><mo>±</mo><mn>11</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq472.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>336</mn><mo>±</mo><mn>11</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq473.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>191</mn><mo>±</mo><mn>9</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq474.gif" /></p></td></tr><tr><td align="left"><p>Background conversion <italic>e</italic></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>53</mn><mo>±</mo><mn>6</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq475.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>35</mn><mo>±</mo><mn>4</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq476.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>19</mn><mo>±</mo><mn>3</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq477.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>15</mn><mo>±</mo><mn>2</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq478.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>424</mn><mo>±</mo><mn>15</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq479.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>227</mn><mo>±</mo><mn>36</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq480.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>185</mn><mo>±</mo><mn>8</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq481.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>116</mn><mo>±</mo><mn>6</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq482.gif" /></p></td></tr><tr><td align="left"><p>Heavy-flavour <italic>e</italic></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>27</mn><mo>±</mo><mn>3</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq483.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>26</mn><mo>±</mo><mn>3</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq484.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3</mn><mo>±</mo><mn>1</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq485.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2</mn><mo>±</mo><mn>1</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq486.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>208</mn><mo>±</mo><mn>8</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq487.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>188</mn><mo>±</mo><mn>8</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq488.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>20</mn><mo>±</mo><mn>3</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq489.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>11</mn><mo>±</mo><mn>2</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq490.gif" /></p></td></tr><tr><td align="left"><p>Other <italic>e</italic></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2</mn><mo>±</mo><mn>2</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq491.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0</mn><mo>±</mo><mn>0</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq492.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1</mn><mo>±</mo><mn>1</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq493.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0</mn><mo>±</mo><mn>0</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq494.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>48</mn><mo>±</mo><mn>9</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq495.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>5</mn><mo>±</mo><mn>1</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq496.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>19</mn><mo>±</mo><mn>3</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq497.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2</mn><mo>±</mo><mn>1</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq498.gif" /></p></td></tr><tr><td align="left"><p>Heavy-flavour <math xmlns="http://www.w3.org/1998/Math/MathML"><mi xmlns="">μ</mi></math><inline-graphic href="10052_2020_7907_Article_IEq499.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>50</mn><mo>±</mo><mn>5</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq500.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>46</mn><mo>±</mo><mn>5</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq501.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>8</mn><mo>±</mo><mn>2</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq502.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2</mn><mo>±</mo><mn>1</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq503.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>434</mn><mo>±</mo><mn>14</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq504.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>335</mn><mo>±</mo><mn>12</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq505.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>79</mn><mo>±</mo><mn>6</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq506.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>27</mn><mo>±</mo><mn>4</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq507.gif" /></p></td></tr><tr><td align="left"><p>Other <math xmlns="http://www.w3.org/1998/Math/MathML"><mi xmlns="">μ</mi></math><inline-graphic href="10052_2020_7907_Article_IEq508.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>11</mn><mo>±</mo><mn>2</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq509.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2</mn><mo>±</mo><mn>1</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq510.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4</mn><mo>±</mo><mn>1</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq511.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0</mn><mo>±</mo><mn>0</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq512.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>54</mn><mo>±</mo><mn>29</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq513.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>151</mn><mo>±</mo><mn>126</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq514.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>46</mn><mo>±</mo><mn>4</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq515.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>11</mn><mo>±</mo><mn>2</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq516.gif" /></p></td></tr><tr><td align="left"><p>Total misidentified</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>201</mn><mo>±</mo><mn>10</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq517.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>149</mn><mo>±</mo><mn>8</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq518.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>69</mn><mo>±</mo><mn>5</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq519.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>40</mn><mo>±</mo><mn>4</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq520.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1761</mn><mo>±</mo><mn>41</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq521.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1266</mn><mo>±</mo><mn>132</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq522.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>684</mn><mo>±</mo><mn>16</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq523.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>358</mn><mo>±</mo><mn>12</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq524.gif" /></p></td></tr><tr><td align="left"><p>Wrong-sign prompt</p></td><td align="left"><p>–</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>24</mn><mo>±</mo><mn>3</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq525.gif" /></p></td><td align="left"><p>–</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>12</mn><mo>±</mo><mn>2</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq526.gif" /></p></td><td align="left"><p>–</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>224</mn><mo>±</mo><mn>9</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq527.gif" /></p></td><td align="left"><p>–</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>113</mn><mo>±</mo><mn>6</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq528.gif" /></p></td></tr><tr><td align="left"><p>Right-sign prompt</p></td><td align="left"><p>–</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>21</mn><mo>±</mo><mn>1</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq529.gif" /></p></td><td align="left"><p>–</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>9</mn><mo>±</mo><mn>0</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq530.gif" /></p></td><td align="left"><p>–</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>195</mn><mo>±</mo><mn>4</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq531.gif" /></p></td><td align="left"><p>–</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>88</mn><mo>±</mo><mn>1</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq532.gif" /></p></td></tr><tr><td align="left"><p>Total</p></td><td align="left"><p>–</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>194</mn><mo>±</mo><mn>9</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq533.gif" /></p></td><td align="left"><p>–</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>61</mn><mo>±</mo><mn>4</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq534.gif" /></p></td><td align="left"><p>–</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1685</mn><mo>±</mo><mn>132</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq535.gif" /></p></td><td align="left"><p>–</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>560</mn><mo>±</mo><mn>13</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq536.gif" /></p></td></tr><tr><td align="left"><p>Data</p></td><td align="left"><p>–</p></td><td align="left"><p>167</p></td><td align="left"><p>–</p></td><td align="left"><p>55</p></td><td align="left"><p>–</p></td><td align="left"><p>1655</p></td><td align="left"><p>–</p></td><td align="left"><p>551</p></td></tr></tbody></table> </ephtml> </p> <p>The ratios <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>R</mi><mi>j</mi></msub></math> </ephtml> in Eq. (<reflink idref="bib6" id="ref83">6</reflink>) were evaluated to be <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>R</mi><mn>1</mn></msub><mo>=</mo><mn>1.4</mn><mo>±</mo><mn>0.3</mn></mrow></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>R</mi><mn>2</mn></msub><mo>=</mo><mn>1.7</mn><mo>±</mo><mn>0.9</mn></mrow></math> </ephtml> for the 2015 data sample, and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>R</mi><mn>1</mn></msub><mo>=</mo><mn>1.4</mn><mo>±</mo><mn>0.4</mn></mrow></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>R</mi><mn>2</mn></msub><mo>=</mo><mn>1.9</mn><mo>±</mo><mn>1.0</mn></mrow></math> </ephtml> for the 2016 sample. The uncertainties encompass the range of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>R</mi><mi>j</mi></msub></math> </ephtml> values seen for the major sources of misidentified-lepton events; as can be seen from the entries in Table 3, the opposite- to same-sign event count ratios are different for the main categories, and the uncertainty allows for their relative contributions to be different from that predicted by the baseline simulation. The <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>R</mi><mi>j</mi></msub></math> </ephtml> values seen in the control samples with loosened isolation, and the predictions from alternative <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> simulation samples using Pythia6 or Herwig7 instead of Pythia8 hadronisation were also considered. A conservative 50% uncertainty in the prompt lepton same-sign contribution was also taken into account, covering the mismodelling of electron charge misidentification in simulation and the uncertainties in the predicted cross-sections for <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo>+</mo><mi>V</mi></mrow></math> </ephtml> and diboson processes. The final misidentified-lepton background estimates for the 2015 and 2016 opposite-sign data samples in the inclusive cross-section analysis are shown in Table 2.</p> <p>Graph: Fig. 3 Distributions of a the electron pT, b the electron |η|, c the muon pT and d the muon |η|, in events with a same-sign eμ pair and at least one b-tagged jet. The simulation prediction is normalised to the same integrated luminosity as the data, and broken down into contributions where both leptons are prompt, or one is a misidentified lepton from a photon conversion originating from a top quark decay or from background, from heavy-flavour decay or from other sources. The statistical uncertainty in the total simulation prediction is significant in some bins, and is shown by the hatching. In the pT distributions, the last bin includes the overflows</p> <p>Figure 4 shows the corresponding same-sign event distributions for the dilepton variables, showing a similar quality of modelling of these kinematic distributions by the simulation as seen for the single-lepton variables in Fig. 3. The <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>R</mi><mn>1</mn><mi>i</mi></msubsup></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>R</mi><mn>2</mn><mi>i</mi></msubsup></math> </ephtml> values in the binned version of Eq. (<reflink idref="bib6" id="ref84">6</reflink>) do not vary in simulation beyond the uncertainties assigned above to the inclusive <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>R</mi><mn>1</mn></msub></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>R</mi><mn>2</mn></msub></math> </ephtml> , so the same relative uncertainties in <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>R</mi><mn>1</mn></msub></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>R</mi><mn>2</mn></msub></math> </ephtml> were also used for the differential analysis, and taken to be correlated across all bins.</p> <p>In the opposite-sign sample, the total non- <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> background fraction from all sources varies significantly as a function of some of the differential variables, but remains dominated by <emph>Wt</emph> events in all bins. It reaches around 20% in the one <emph>b</emph>-tag sample and 10% of the two <emph>b</emph>-tag sample at the high ends of the single-lepton <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>ℓ</mi></msubsup></math> </ephtml> and dilepton <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mrow><mi>e</mi><mi>μ</mi></mrow></msubsup></math> </ephtml> distributions, but varies little with lepton <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>η</mi><mi>ℓ</mi></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> .</p> <p>Graph: Fig. 4 Distributions of a the dilepton pTeμ, b invariant mass meμ, c rapidity |yeμ|, d azimuthal angle difference Δϕeμ, e lepton pT sum pTe+pTμ and f lepton energy sum Ee+Eμ, in events with a same-sign eμ pair and at least one b-tagged jet. The simulation prediction is normalised to the same integrated luminosity as the data, and broken down into contributions where both leptons are prompt, or one is a misidentified lepton from a photon conversion originating from a top quark decay or from background, from heavy-flavour decay or from other sources. The statistical uncertainty in the total simulation prediction is significant in some bins, and is shown by the hatching. In the pTeμ, meμ, pTe+pTμ and Ee+Eμ distributions, the last bin includes the overflows</p> <hd id="AN0144642803-9">Validation of the differential measurements</hd> <p>A set of tests using pseudo-experiment datasets generated from simulation were used to validate the analysis procedures for the differential measurements, as documented in detail for the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>8</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> analysis [[<reflink idref="bib29" id="ref85">29</reflink>]]. These tests demonstrated that the method is unbiased and correctly estimates the statistical uncertainties in each bin of each distribution. Figure 5 shows examples for the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>ℓ</mi></msubsup></math> </ephtml> , <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mrow><mi>e</mi><mi>μ</mi></mrow></msubsup></math> </ephtml> , <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>η</mi><mi>ℓ</mi></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>y</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> distributions. The filled black points show the relative differences between the mean normalised differential cross-sections obtained from 1000 pseudo-experiments and the true cross-sections in each bin, divided by the true cross-sections to give fractional differences. The pseudo-experiments were generated from a reference <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> sample, and the reference sample was also used to determine the values of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>G</mi><mrow><mi>e</mi><mi>μ</mi></mrow><mi>i</mi></msubsup></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>C</mi><mi>b</mi><mi>i</mi></msubsup></math> </ephtml> in each bin <emph>i</emph> of the distributions. The compatibility of the filled black points with zero within the statistical uncertainty of the reference sample confirms that the method is unbiased for this sample. The open red points and dotted lines show the mean pseudo-experiment results and true values for an alternative sample with different underlying distributions, again expressed as fractional deviations from the true cross-sections in the reference sample, and obtained using <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>G</mi><mrow><mi>e</mi><mi>μ</mi></mrow><mi>i</mi></msubsup></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>C</mi><mi>b</mi><mi>i</mi></msubsup></math> </ephtml> values from the reference sample. The alternative samples were chosen in order to produce a large variation in the distribution under test. An independent <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> simulation sample with <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>m</mi><mi>t</mi></msub><mo>=</mo><mn>175</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math> </ephtml> was used for the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>ℓ</mi></msubsup></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mrow><mi>e</mi><mi>μ</mi></mrow></msubsup></math> </ephtml> distributions, and the baseline <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> sample generated with NNPDF3.0 was reweighted to the predictions of the CT14 PDF set [[<reflink idref="bib74" id="ref86">74</reflink>]] for <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>η</mi><mi>ℓ</mi></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>y</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> . In all cases, the results are consistent with the true values within the statistical uncertainties of the alternative samples, demonstrating that the simple bin-by-bin correction procedure correctly recovers the alternative distributions, without the need for iteration or a matrix-based unfolding technique. Similar results were obtained for the analogous validation tests performed on the double-differential cross-section measurements. The various distributions shown in Fig. 5 also illustrate the sensitivity of the normalised differential cross-sections to <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>m</mi><mi>t</mi></msub></math> </ephtml> and different PDF sets.</p> <p>Graph: Fig. 5 Results of pseudo-experiment studies on simulated events for the extraction of the normalised differential cross-section distributions for apTℓ, bpTeμ, c|ηℓ| and d|yeμ|, shown as relative deviations (σ-σref)/σref from the reference cross-section values in the Powheg + Pythia6 CT10 (a, b) or Powheg + Pythia8 NNPDF3.0 (c, d) samples with mt=172.5Ge. The black filled points show the mean deviations from the reference values of the results from pseudo-data samples generated with the reference simulation sample, with error bars indicating the uncertainties due to the limited number of simulated events. The cyan shaded bands indicate the expected statistical uncertainties for a single sample corresponding to the data integrated luminosity. The open red points show the mean deviations from the reference values obtained from pseudo-experiments generated from an alternative simulation sample with mt=175Ge (a, b) or by reweighting the baseline sample to the CT14 PDF (c, d). The red error bars represent the uncertainty due to the limited size of these alternative samples, and the red dotted lines show the true deviations from the reference in the alternative samples</p> <hd id="AN0144642803-10">Systematic uncertainties</hd> <p>Systematic uncertainties in the measured inclusive cross-section arise from uncertainties in the input quantities <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>ϵ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msub></math> </ephtml> , <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>C</mi><mi>b</mi></msub></math> </ephtml> , <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>N</mi><mn>1</mn><mi mathvariant="normal">bkg</mi></msubsup></math> </ephtml> , <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>N</mi><mn>2</mn><mi mathvariant="normal">bkg</mi></msubsup></math> </ephtml> and <emph>L</emph> appearing in Eq. (<reflink idref="bib1" id="ref87">1</reflink>), and the corresponding quantities in Eq. (<reflink idref="bib2" id="ref88">2</reflink>) for the differential cross-sections. Each source of systematic uncertainty was evaluated by changing all relevant input quantities coherently and re-solving the tagging equations, thus taking into account systematic correlations between the different inputs (and between different bins in the differential analysis). The sources of systematic uncertainty are divided into the five groups discussed below, and are shown in detail for the inclusive and fiducial <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> cross-sections in Table 4. The uncertainties are shown in groups for each bin of the single- and double-differential cross-sections in Tables 15, 16, 17, 18, 19, 20, 21, 22, 23, 24, and the uncertainties for the normalised single-differential cross-sections are also shown in Fig. 6.</p> <p>Breakdown of the relative systematic uncertainties in <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>ϵ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msub></math> </ephtml> , <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>G</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msub></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>C</mi><mi>b</mi></msub></math> </ephtml> , and the statistical, systematic (excluding luminosity and beam energy) and total uncertainties in the inclusive and fiducial <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> cross-section measurements. The five groups of systematic uncertainties corresponding to the discussion in Sects. 5.1 to 5.5 are indicated in the leftmost column</p> <p> <ephtml> <table frame="hsides" rules="groups"><thead><tr><th align="left" rowspan="3" /><th align="left" rowspan="2"><p>Uncertainty source</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi mathvariant="normal">Δ</mi><msub><mi>ϵ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msub><mo stretchy="false">/</mo><msub><mi>ϵ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msub></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq609.gif" /></p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi mathvariant="normal">Δ</mi><msub><mi>G</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msub><mo stretchy="false">/</mo><msub><mi>G</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msub></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq610.gif" /></p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi mathvariant="normal">Δ</mi><msub><mi>C</mi><mi>b</mi></msub><mo stretchy="false">/</mo><msub><mi>C</mi><mi>b</mi></msub></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq611.gif" /></p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi mathvariant="normal">Δ</mi><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub><mo stretchy="false">/</mo><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq612.gif" /></p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi mathvariant="normal">Δ</mi><msubsup><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow><mi mathvariant="normal">fid</mi></msubsup><mo stretchy="false">/</mo><msubsup><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow><mi mathvariant="normal">fid</mi></msubsup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq613.gif" /></p></th></tr><tr><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th></tr><tr><th align="left"><p>Data statistics</p></th><th align="left" /><th align="left" /><th align="left" /><th align="left"><p>0.44</p></th><th align="left"><p>0.44</p></th></tr></thead><tbody><tr><td align="left" rowspan="6"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq614.gif" /> mod.</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq615.gif" /> generator</p></td><td align="left"><p>0.38</p></td><td align="left"><p>0.05</p></td><td align="left"><p>0.05</p></td><td align="left"><p>0.43</p></td><td align="left"><p>0.10</p></td></tr><tr><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq616.gif" /> hadronisation</p></td><td align="left"><p>0.24</p></td><td align="left"><p>0.42</p></td><td align="left"><p>0.25</p></td><td align="left"><p>0.49</p></td><td align="left"><p>0.67</p></td></tr><tr><td align="left"><p>Initial/final-state radiation</p></td><td align="left"><p>0.30</p></td><td align="left"><p>0.26</p></td><td align="left"><p>0.16</p></td><td align="left"><p>0.45</p></td><td align="left"><p>0.41</p></td></tr><tr><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq617.gif" /> heavy-flavour production</p></td><td align="left"><p>0.01</p></td><td align="left"><p>0.01</p></td><td align="left"><p>0.26</p></td><td align="left"><p>0.26</p></td><td align="left"><p>0.26</p></td></tr><tr><td align="left"><p>Parton distribution functions</p></td><td align="left"><p>0.44</p></td><td align="left"><p>0.05</p></td><td align="left"><p>–</p></td><td align="left"><p>0.45</p></td><td align="left"><p>0.07</p></td></tr><tr><td align="left"><p>Simulation statistics</p></td><td align="left"><p>0.22</p></td><td align="left"><p>0.15</p></td><td align="left"><p>0.17</p></td><td align="left"><p>0.22</p></td><td align="left"><p>0.18</p></td></tr><tr><td align="left" rowspan="10"><p>Lept.</p></td><td align="left"><p>Electron energy scale</p></td><td align="left"><p>0.06</p></td><td align="left"><p>0.06</p></td><td align="left"><p>–</p></td><td align="left"><p>0.06</p></td><td align="left"><p>0.06</p></td></tr><tr><td align="left"><p>Electron energy resolution</p></td><td align="left"><p>0.01</p></td><td align="left"><p>0.01</p></td><td align="left"><p>–</p></td><td align="left"><p>0.01</p></td><td align="left"><p>0.01</p></td></tr><tr><td align="left"><p>Electron identification</p></td><td align="left"><p>0.34</p></td><td align="left"><p>0.34</p></td><td align="left"><p>–</p></td><td align="left"><p>0.37</p></td><td align="left"><p>0.37</p></td></tr><tr><td align="left"><p>Electron charge mis-id</p></td><td align="left"><p>0.09</p></td><td align="left"><p>0.09</p></td><td align="left"><p>–</p></td><td align="left"><p>0.10</p></td><td align="left"><p>0.10</p></td></tr><tr><td align="left"><p>Electron isolation</p></td><td align="left"><p>0.22</p></td><td align="left"><p>0.22</p></td><td align="left"><p>–</p></td><td align="left"><p>0.24</p></td><td align="left"><p>0.24</p></td></tr><tr><td align="left"><p>Muon momentum scale</p></td><td align="left"><p>0.03</p></td><td align="left"><p>0.03</p></td><td align="left"><p>–</p></td><td align="left"><p>0.03</p></td><td align="left"><p>0.03</p></td></tr><tr><td align="left"><p>Muon momentum resolution</p></td><td align="left"><p>0.01</p></td><td align="left"><p>0.01</p></td><td align="left"><p>–</p></td><td align="left"><p>0.01</p></td><td align="left"><p>0.01</p></td></tr><tr><td align="left"><p>Muon identification</p></td><td align="left"><p>0.28</p></td><td align="left"><p>0.28</p></td><td align="left"><p>–</p></td><td align="left"><p>0.30</p></td><td align="left"><p>0.30</p></td></tr><tr><td align="left"><p>Muon isolation</p></td><td align="left"><p>0.16</p></td><td align="left"><p>0.16</p></td><td align="left"><p>–</p></td><td align="left"><p>0.18</p></td><td align="left"><p>0.18</p></td></tr><tr><td align="left"><p>Lepton trigger</p></td><td align="left"><p>0.13</p></td><td align="left"><p>0.13</p></td><td align="left"><p>–</p></td><td align="left"><p>0.14</p></td><td align="left"><p>0.14</p></td></tr><tr><td align="left" rowspan="5"><p>Jet/<italic>b</italic></p></td><td align="left"><p>Jet energy scale</p></td><td align="left"><p>0.02</p></td><td align="left"><p>0.02</p></td><td align="left"><p>0.06</p></td><td align="left"><p>0.03</p></td><td align="left"><p>0.03</p></td></tr><tr><td align="left"><p>Jet energy resolution</p></td><td align="left"><p>0.01</p></td><td align="left"><p>0.01</p></td><td align="left"><p>0.04</p></td><td align="left"><p>0.01</p></td><td align="left"><p>0.01</p></td></tr><tr><td align="left"><p>Pileup jet veto</p></td><td align="left"><p>–</p></td><td align="left"><p>–</p></td><td align="left"><p>–</p></td><td align="left"><p>0.02</p></td><td align="left"><p>0.02</p></td></tr><tr><td align="left"><p><italic>b</italic>-tagging efficiency</p></td><td align="left"><p>–</p></td><td align="left"><p>–</p></td><td align="left"><p>0.04</p></td><td align="left"><p>0.20</p></td><td align="left"><p>0.20</p></td></tr><tr><td align="left"><p><italic>b</italic>-tag mistagging</p></td><td align="left"><p>–</p></td><td align="left"><p>–</p></td><td align="left"><p>0.06</p></td><td align="left"><p>0.06</p></td><td align="left"><p>0.06</p></td></tr><tr><td align="left" rowspan="8"><p>Bkg.</p></td><td align="left"><p>Single-top cross–section</p></td><td align="left"><p>–</p></td><td align="left"><p>–</p></td><td align="left"><p>–</p></td><td align="left"><p>0.52</p></td><td align="left"><p>0.52</p></td></tr><tr><td align="left"><p>Single-top/<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq618.gif" /> interference</p></td><td align="left"><p>–</p></td><td align="left"><p>–</p></td><td align="left"><p>–</p></td><td align="left"><p>0.15</p></td><td align="left"><p>0.15</p></td></tr><tr><td align="left"><p>Single-top modelling</p></td><td align="left"><p>–</p></td><td align="left"><p>–</p></td><td align="left"><p>–</p></td><td align="left"><p>0.34</p></td><td align="left"><p>0.34</p></td></tr><tr><td align="left"><p><italic>Z</italic>+jets extrapolation</p></td><td align="left"><p>–</p></td><td align="left"><p>–</p></td><td align="left"><p>–</p></td><td align="left"><p>0.09</p></td><td align="left"><p>0.09</p></td></tr><tr><td align="left"><p>Diboson cross-sections</p></td><td align="left"><p>–</p></td><td align="left"><p>–</p></td><td align="left"><p>–</p></td><td align="left"><p>0.02</p></td><td align="left"><p>0.02</p></td></tr><tr><td align="left"><p>Diboson modelling</p></td><td align="left"><p>–</p></td><td align="left"><p>–</p></td><td align="left"><p>–</p></td><td align="left"><p>0.03</p></td><td align="left"><p>0.03</p></td></tr><tr><td align="left"><p>Misidentified leptons</p></td><td align="left"><p>–</p></td><td align="left"><p>–</p></td><td align="left"><p>–</p></td><td align="left"><p>0.43</p></td><td align="left"><p>0.43</p></td></tr><tr><td align="left"><p>Analysis systematics</p></td><td align="left"><p>0.91</p></td><td align="left"><p>0.75</p></td><td align="left"><p>0.44</p></td><td align="left"><p>1.39</p></td><td align="left"><p>1.31</p></td></tr><tr><td align="left" rowspan="3"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>L</mi><mo stretchy="false">/</mo><msub><mi>E</mi><mi mathvariant="normal">b</mi></msub></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq619.gif" /></p></td><td align="left"><p>Integrated luminosity</p></td><td align="left"><p>–</p></td><td align="left"><p>–</p></td><td align="left"><p>–</p></td><td align="left"><p>1.90</p></td><td align="left"><p>1.90</p></td></tr><tr><td align="left"><p>Beam energy</p></td><td align="left"><p>–</p></td><td align="left"><p>–</p></td><td align="left"><p>–</p></td><td align="left"><p>0.23</p></td><td align="left"><p>0.23</p></td></tr><tr><td align="left"><p>Total uncertainty</p></td><td align="left"><p>0.91</p></td><td align="left"><p>0.75</p></td><td align="left"><p>0.44</p></td><td align="left"><p>2.40</p></td><td align="left"><p>2.36</p></td></tr></tbody></table> </ephtml> </p> <p>Graph: Fig. 6 Relative uncertainties in the measured normalised differential cross-sections coming from data statistics, tt¯ modelling, leptons, jets and background, as a function of each lepton or dilepton differential variable. The total uncertainty is shown by the thick black lines, and also includes small contributions from the integrated luminosity and LHC beam energy uncertainties</p> <hd id="AN0144642803-11">tt¯ modelling</hd> <p>The uncertainties in <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>ϵ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msub></math> </ephtml> , <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>G</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msub></math> </ephtml> , <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>G</mi><mrow><mi>e</mi><mi>μ</mi></mrow><mi>i</mi></msubsup></math> </ephtml> , <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>C</mi><mi>b</mi></msub></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>C</mi><mi>b</mi><mi>i</mi></msubsup></math> </ephtml> (and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>f</mi><mrow><mi mathvariant="normal">no</mi><mo>-</mo><mi>τ</mi></mrow><mi>i</mi></msubsup></math> </ephtml> for the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mi>τ</mi></math> </ephtml> -corrected cross-sections) were evaluated using the alternative <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> samples described in Sect. 2. The <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> generator uncertainty was determined by comparing the baseline Powheg + Pythia8 sample with aMC@NLO + Pythia8. The parton shower, hadronisation and underlying event uncertainty (referred to as 'hadronisation' below) was evaluated by comparing the baseline with Powheg + Herwig7. The initial/final-state radiation uncertainty was evaluated as half the difference between the Powheg + Pythia8 model variations with more or less parton-shower radiation; as discussed in Sect. 2, these samples also include variations of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>μ</mi><mi mathvariant="normal">F</mi></msub></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>μ</mi><mi mathvariant="normal">R</mi></msub></math> </ephtml> . As shown in Table 4, the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> generator uncertainty is larger for <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>ϵ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msub></math> </ephtml> than for <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>G</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msub></math> </ephtml> , as the Powheg + Pythia8 and aMC@NLO + Pythia8 samples predict different particle-level acceptances <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>A</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msub></math> </ephtml> . In contrast, the differences in <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>A</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msub></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>G</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msub></math> </ephtml> for the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> hadronisation uncertainty have opposite signs, leading to a smaller shift in <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>ϵ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msub></math> </ephtml> than in <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>G</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msub></math> </ephtml> . In the differential analyses, the bin-by-bin shifts in <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>G</mi><mrow><mi>e</mi><mi>μ</mi></mrow><mi>i</mi></msubsup></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>C</mi><mi>b</mi><mi>i</mi></msubsup></math> </ephtml> were fitted with polynomial functions to reduce statistical fluctuations. All these comparisons were carried out without applying the lepton isolation requirements, as the isolation efficiencies were measured in situ in data as discussed in Sect. 5.2, and the simulation was only used to predict the lepton reconstruction, identification and overlap removal uncertainties. This procedure also reduces the sensitivity to the modelling of hadronisation, the underlying event and colour reconnection.</p> <p>The values of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>C</mi><mi>b</mi></msub></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>C</mi><mi>b</mi><mi>i</mi></msubsup></math> </ephtml> are sensitive to the fraction of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> events with extra <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>b</mi><mover accent="true"><mrow><mi>b</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> or <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>c</mi><mover accent="true"><mrow><mi>c</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> pairs. Such <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> plus heavy-flavour production gives rise to events with three or more <emph>b</emph>-tagged jets; as can be seen from Fig. 1a and also measured in a dedicated analysis [[<reflink idref="bib75" id="ref89">75</reflink>]], this rate is underestimated by the available <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> models that only produce extra <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>b</mi><mover accent="true"><mrow><mi>b</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> or <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>c</mi><mover accent="true"><mrow><mi>c</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> pairs through the parton shower. The potential effect on <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>C</mi><mi>b</mi></msub></math> </ephtml> was studied by reweighting the baseline Powheg + Pythia8 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> sample so as to increase the fraction of events with at least three <emph>b</emph>-jets at generator level by 40%, an enhancement which reproduces both the rate of events with three <emph>b</emph>-tags and the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mi>η</mi></math> </ephtml> distributions of the third highest- <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml><emph>b</emph>-tagged jet in these events. The resulting shifts in <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>C</mi><mi>b</mi></msub></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>C</mi><mi>b</mi><mi>i</mi></msubsup></math> </ephtml> were assigned as additional systematic uncertainties due to the modelling of heavy-flavour production in <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> events.</p> <p>Parton distribution function uncertainties were evaluated by reweighting the baseline Powheg + Pythia8 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> sample using generator weights associated with each of the 100 variations (replicas) provided by the NNPDF3.0 authors [[<reflink idref="bib44" id="ref90">44</reflink>]], and calculating the RMS of the changes induced in <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>ϵ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msub></math> </ephtml> , <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>G</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msub></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>G</mi><mrow><mi>e</mi><mi>μ</mi></mrow><mi>i</mi></msubsup></math> </ephtml> . The resulting uncertainties are 0.45% in <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> , but less than 0.1% in <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow><mi mathvariant="normal">fid</mi></msubsup></math> </ephtml> , as variations of the PDF mainly affect the acceptance rather than the reconstruction efficiency. Similar uncertainties were found for the PDF4LHC15_NLO_30 meta-PDF [[<reflink idref="bib76" id="ref91">76</reflink>]], which is based on a Monte Carlo combination of the NNPDF3.0, CT14 [[<reflink idref="bib74" id="ref92">74</reflink>]] and MMHT14 [[<reflink idref="bib77" id="ref93">77</reflink>]] PDF sets. The central values from all these PDF sets lie within the uncertainty band obtained from NNPDF3.0.</p> <p>The prediction for <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>ϵ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msub></math> </ephtml> is also sensitive to the assumed value of the top quark mass, as a heavier top quark increases the average lepton <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> and makes their <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mo stretchy="false">|</mo><mi>η</mi><mo stretchy="false">|</mo></mrow></math> </ephtml> slightly more central. This effect was evaluated using <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> simulation samples with <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>m</mi><mi>t</mi></msub></math> </ephtml> variations from 170 to 177.5 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> , giving a relative change in <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>ϵ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msub></math> </ephtml> of 0.3% for a 1 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> change in <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>m</mi><mi>t</mi></msub></math> </ephtml> . The effect is partially counterbalanced by changes in the <emph>Wt</emph> background prediction, which decreases with increasing <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>m</mi><mi>t</mi></msub></math> </ephtml> . By convention, the inclusive <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> cross-section <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> is quoted at a fixed top quark mass value, but a <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mo>±</mo><mn>1</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math> </ephtml> variation in <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>m</mi><mi>t</mi></msub></math> </ephtml> is included in the uncertainties for the lepton differential distributions.</p> <p>The total <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> modelling uncertainties also include the small contributions due to the limited size of the baseline <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> simulation sample, and are shown for the differential distributions by the green dotted lines in Fig. 6.</p> <hd id="AN0144642803-12">Lepton identification and measurement</hd> <p>The modelling of the electron and muon identification efficiencies was studied using <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>Z</mi><mo stretchy="false">→</mo><mi>e</mi><mi>e</mi><mo stretchy="false">/</mo><mi>μ</mi><mi>μ</mi></mrow></math> </ephtml> events, as described in Refs. [[<reflink idref="bib63" id="ref94">63</reflink>]]. Small corrections were applied to the simulation, and the correlations in the associated systematic uncertainties as a function of lepton <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mi>η</mi></math> </ephtml> were taken into account and propagated to all differential distributions. Similar procedures were used to measure the electron and muon trigger efficiencies with <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>Z</mi><mo stretchy="false">→</mo><mi>e</mi><mi>e</mi><mo stretchy="false">/</mo><mi>μ</mi><mi>μ</mi></mrow></math> </ephtml> decays. Since only one lepton was required to pass the trigger requirements in order to accept the event, the trigger efficiencies for events passing the offline selection are high, around 97% for 2015 data and 94% for 2016 data. Most of the efficiency loss comes from events where one lepton has a transverse momentum below the trigger threshold and the other lepton is above the threshold but fails the trigger selection. The electron charge misidentification probability was measured as a function of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mo stretchy="false">|</mo><mi>η</mi><mo stretchy="false">|</mo></mrow></math> </ephtml> using the ratio of same- to opposite-sign reconstructed <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>Z</mi><mo stretchy="false">→</mo><mi>e</mi><mi>e</mi></mrow></math> </ephtml> events, and the full difference between data and simulation, which is only significant for forward electrons with <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mo stretchy="false">|</mo><mi>η</mi><mo stretchy="false">|</mo><mo>></mo><mn>1.5</mn></mrow></math> </ephtml> , was assigned as an uncertainty. The electron and muon energy/momentum scales and resolutions were determined using <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>Z</mi><mo stretchy="false">→</mo><mi>e</mi><mi>e</mi><mo stretchy="false">/</mo><mi>μ</mi><mi>μ</mi></mrow></math> </ephtml> , <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>Z</mi><mo stretchy="false">→</mo><mi>ℓ</mi><mi>ℓ</mi><mi>γ</mi></mrow></math> </ephtml> , <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>J</mi><mo stretchy="false">/</mo><mi>ψ</mi><mo stretchy="false">→</mo><mi>e</mi><mi>e</mi><mo stretchy="false">/</mo><mi>μ</mi><mi>μ</mi></mrow></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi mathvariant="normal">Υ</mi><mo stretchy="false">→</mo><mi>μ</mi><mi>μ</mi></mrow></math> </ephtml> decays [[<reflink idref="bib64" id="ref95">64</reflink>], [<reflink idref="bib78" id="ref96">78</reflink>]], and the residual uncertainties are typically much smaller than those associated with the lepton efficiency measurements.</p> <p>The lepton isolation efficiencies were measured directly in the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> -dominated <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>e</mi><mi>μ</mi></mrow></math> </ephtml> plus <emph>b</emph>-tagged jet samples, by determining the fractions of events where either the electron or muon fails the isolation cut, as functions of lepton <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> and separately for the barrel ( <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mo stretchy="false">|</mo><mi>η</mi><mo stretchy="false">|</mo><mo><</mo><mn>1.5</mn></mrow></math> </ephtml> ) and forward regions. The samples of leptons failing isolation cuts have significant contamination from misidentified leptons, reaching up to 10% in the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>e</mi><mi>μ</mi></mrow></math> </ephtml> plus two <emph>b</emph>-tagged jet sample at low lepton <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> , and up to 50% in the one <emph>b</emph>-tagged jet sample, but in both cases decreasing strongly with increasing lepton <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> . The results were corrected for this contamination, estimated from data with the aid of leptons with large impact parameter significance ( <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msub><mi>d</mi><mn>0</mn></msub><mrow><mo stretchy="false">|</mo><mo stretchy="false">/</mo></mrow><msub><mi>σ</mi><msub><mi>d</mi><mn>0</mn></msub></msub><mo>></mo><mn>5</mn></mrow></math> </ephtml> ), that provide a control sample enriched in misidentified leptons. Templates for the impact parameter significance distributions of misidentified leptons were obtained from the same-sign <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>e</mi><mi>μ</mi></mrow></math> </ephtml> samples, subtracting estimated prompt lepton contributions using simulation. The total uncertainties on the measured isolation efficiencies are up to 0.9% for electrons and 0.6% for muons at low lepton <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> , dominated by the dependence on the choice of impact parameter significance cut, and reduce to 0.1% at high <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> , where the isolation efficiency is around 98% and the misidentified lepton contributions are very small. The method was validated by using the various alternative <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> simulation samples (which predict different isolation efficiencies) as pseudo-data, and by explicitly changing the lepton isolation efficiencies in simulation and verifying that the measurement procedure recovered the changes.</p> <p>The isolation efficiencies measured on data are shown in Fig. 7, together with the prediction from simulation. The baseline <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> simulation sample gives a good modelling of the muon isolation efficiency, but underestimates the electron isolation efficiency in data by up to 1% at low lepton <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> , leading to a total correction of about 0.4% for <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>ϵ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msub></math> </ephtml> . The residual uncertainties on the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> -integrated corrections are around 0.2% for both electrons and muons, dominated by the subtraction of misidentified-lepton background at low <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> . For comparison, the differing lepton isolation efficiency predictions from the various <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> simulation samples would lead to differences in <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>ϵ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msub></math> </ephtml> of up to about 0.4%. The corresponding corrections as a function of lepton <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mo stretchy="false">|</mo><mi>η</mi><mo stretchy="false">|</mo></mrow></math> </ephtml> were propagated to the values of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>G</mi><mrow><mi>e</mi><mi>μ</mi></mrow><mi>i</mi></msubsup></math> </ephtml> in each bin of the differential distributions, and also applied to the estimates for the dominant <emph>Wt</emph> background. The total lepton-related uncertainties are shown by the blue dot-dashed lines in Fig. 6.</p> <p>Graph: Fig. 7 Lepton isolation efficiencies for a electrons and b muons measured in the tt¯-dominated eμ plus b-tagged jets sample. The data measurements are shown by the black points with error bars indicating the total uncertainty, and the predictions of the baseline simulation with Powheg + Pythia8tt¯ events plus background shown by the cyan bands with width indicating the statistical uncertainty. The measurements are shown for eight bins of lepton pT in the barrel region (|η|<1.5) and three bins in the forward region (|η|>1.5)</p> <hd id="AN0144642803-13">Jet measurement and b-tagging</hd> <p>Uncertainties in jet reconstruction and calibration affect the estimates of the background contributions from <emph>Wt</emph> and diboson events, and the values of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>C</mi><mi>b</mi></msub></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>C</mi><mi>b</mi><mi>i</mi></msubsup></math> </ephtml> . They also have a very small effect on <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>ϵ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msub></math> </ephtml> , <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>G</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msub></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>G</mi><mrow><mi>e</mi><mi>μ</mi></mrow><mi>i</mi></msubsup></math> </ephtml> due to the removal of leptons within <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi mathvariant="normal">Δ</mi><msub><mi>R</mi><mi>y</mi></msub><mo>=</mo><mn>0.4</mn></mrow></math> </ephtml> of selected jets. The jet energy scale was determined using a combination of simulation, test beam and in situ measurements [[<reflink idref="bib68" id="ref97">68</reflink>]] and the corresponding uncertainties were evaluated using a model with 20 independent uncertainty components. The jet energy resolution was measured using Run 1 data [[<reflink idref="bib79" id="ref98">79</reflink>]] and the resulting uncertainties were extrapolated to the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> data samples. The modelling of the JVT requirement used to reject jets coming from pileup was evaluated using jets in <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>Z</mi><mo stretchy="false">→</mo><mi>μ</mi><mi>μ</mi></mrow></math> </ephtml> events [[<reflink idref="bib69" id="ref99">69</reflink>]].</p> <p>The efficiency for <emph>b</emph>-tagging jets in <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> events was extracted from the data via Eq. (<reflink idref="bib1" id="ref100">1</reflink>), but simulation was used to predict the numbers of <emph>b</emph>-tagged jets in <emph>Wt</emph> and diboson background events. The values of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>C</mi><mi>b</mi></msub></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>C</mi><mi>b</mi><mi>i</mi></msubsup></math> </ephtml> also depend weakly on the efficiencies for tagging both heavy- and light-flavoured jets. The modelling of the <emph>b</emph>-tagging performance in simulation was corrected using scale factors determined using dileptonic <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> events for <emph>b</emph>-jets [[<reflink idref="bib70" id="ref101">70</reflink>]], single-lepton <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> events for charm jets [[<reflink idref="bib80" id="ref102">80</reflink>]], and dijet events for light-quark and gluon jets [[<reflink idref="bib81" id="ref103">81</reflink>]]. The corresponding uncertainties were propagated to the background and correlation coefficient estimates. The uncertainties related to jets and <emph>b</emph>-tagging are shown by the purple dashed lines in Fig. 6, and are dominated by the effects of <emph>b</emph>-tagging uncertainties on the background estimates.</p> <hd id="AN0144642803-14">Background modelling</hd> <p>The normalisation of the <emph>Wt</emph> background was varied by 5.3%, corresponding to the PDF and QCD scale uncertainties on the approximate NNLO cross-section prediction discussed in Sect. 2. The potential effects of interference between the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> and <emph>Wt</emph> final states were assessed by comparing the predictions of Powheg + Pythia6 samples with the diagram removal and diagram subtraction approaches to handling this interference [[<reflink idref="bib54" id="ref104">54</reflink>], [<reflink idref="bib57" id="ref105">57</reflink>], [<reflink idref="bib82" id="ref106">82</reflink>]]. The corresponding uncertainty in the inclusive cross-section result is small, but the diagram subtraction method predicts up to 30% less <emph>Wt</emph> background in the one <emph>b</emph>-tag sample and 60% less in the two <emph>b</emph>-tag sample at the high ends of the lepton <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> and dilepton <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mrow><mi>e</mi><mi>μ</mi></mrow></msubsup></math> </ephtml> , <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></math> </ephtml> , <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>e</mi></msubsup><mo>+</mo><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>μ</mi></msubsup></mrow></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msup><mi>E</mi><mi>e</mi></msup><mo>+</mo><msup><mi>E</mi><mi>μ</mi></msup></mrow></math> </ephtml> distributions, where interference effects become large and dominate the total uncertainty (see Fig. 6). However, a dedicated study of events with two leptons and two <emph>b</emph>-tagged jets [[<reflink idref="bib83" id="ref107">83</reflink>]] suggests that the data lie between the predictions of the models with diagram removal and diagram subtraction in the region where interference effects are important. Further modelling uncertainties were assessed by comparing the predictions from the baseline <emph>Wt</emph> sample with those of aMC@NLO interfaced to Herwig++ [[<reflink idref="bib84" id="ref108">84</reflink>]], with Powheg + Pythia6 samples with more or less parton-shower radiation, and with Powheg + Herwig7, in all cases normalising the total production cross-section to the approximate NNLO prediction. The small background acceptance uncertainties due to variations of the PDFs were evaluated using NNPDF3.0 replicas in the same way as for the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> signal. They were taken to be uncorrelated with the signal PDF uncertainties, but are included in the 'Parton distribution functions' entry in Table 4.</p> <p>Uncertainties in the diboson background were assessed by varying the cross-sections by 6% based on calculations with MCFM [[<reflink idref="bib85" id="ref109">85</reflink>]] using the CT10 PDF set [[<reflink idref="bib18" id="ref110">18</reflink>]], and changing the QCD factorisation, renormalisation, resummation and CKKW matching scales by factors of two up and down within the Sherpa generator. The combined uncertainties amount to 12% of the diboson contribution to the one <emph>b</emph>-tag sample and 33% for the two <emph>b</emph>-tag sample.</p> <p>The backgrounds from <emph>Z</emph>+jets and events with misidentified leptons were estimated using data control samples, and the corresponding uncertainties were evaluated as discussed in Sect. 4.3. The total background-related uncertainties in the normalised differential cross-sections are shown by the red solid lines in Fig. 6, and are dominated by those in the <emph>Wt</emph> background.</p> <hd id="AN0144642803-15">Luminosity and beam energy</hd> <p>The uncertainties in the integrated luminosity are 2.0% for the 2015 and 2.1% for the 2016 datasets, evaluated as discussed in Ref. [[<reflink idref="bib86" id="ref111">86</reflink>]] using a calibration of the LUCID-2 detector [[<reflink idref="bib87" id="ref112">87</reflink>]] obtained from <emph>x</emph>–<emph>y</emph> beam-separation scans in each year. For the inclusive cross-section analysis, the total luminosity uncertainties were broken down into individual components which were each considered correlated or uncorrelated between years, as appropriate, in the combination of the cross-section results from the two datasets [[<reflink idref="bib86" id="ref113">86</reflink>]]. A single luminosity uncertainty of 2.1% in the combined 2015–2016 sample was used for the differential cross-section analysis. In both cases, the luminosity-induced uncertainties in the measured cross-sections are around 10% larger than the uncertainty in the integrated luminosity itself, as the integrated luminosity is needed both for the conversion of the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> event yields to <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> , and in order to normalise the simulation-based estimates of the <emph>Wt</emph> and diboson backgrounds.</p> <p>The LHC beam energy is known to be within 0.1% of the nominal value of exactly 6.5 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> per beam for <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> collisions, based on the LHC magnetic model and comparisons of the revolution frequencies of proton and lead-ion beams [[<reflink idref="bib88" id="ref114">88</reflink>]]. A 0.1% variation in <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msqrt><mi>s</mi></msqrt></math> </ephtml> corresponds to a 0.23% variation in <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> , according to the NNLO+NNLL predictions of Top++ [[<reflink idref="bib14" id="ref115">14</reflink>]]. Following the approach of previous analyses [[<reflink idref="bib7" id="ref116">7</reflink>], [<reflink idref="bib9" id="ref117">9</reflink>]], this uncertainty is included in the experimental uncertainty of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> , allowing the measurement to be compared with theoretical predictions for <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> at exactly <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> . The beam energy uncertainty also affects the predictions for both the absolute and normalised differential distributions, as e.g. the lepton <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> distributions become slightly harder and the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>η</mi><mi>ℓ</mi></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> distributions slightly more forward as <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msqrt><mi>s</mi></msqrt></math> </ephtml> increases. These shifts were evaluated by reweighting the aMC@NLO + Pythia8 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> sample using PDF weights calculated using LHAPDF [[<reflink idref="bib89" id="ref118">89</reflink>]] so as to vary the effective <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msqrt><mi>s</mi></msqrt></math> </ephtml> by <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mo>±</mo><mn>0.1</mn></mrow></math> </ephtml> %, and the resulting uncertainties were included in the differential cross-section results. The combined effects of the luminosity and beam energy uncertainties on the normalised differential cross-sections are listed in Tables 15, 16, 17, 18, and are at most 0.3%, always small compared with the other systematic and statistical uncertainties of the measurements.</p> <hd id="AN0144642803-16">Inclusive cross-section results and interpretation</hd> <p>The results of the inclusive <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> cross-section analysis are given in Sect. 6.1, followed by the extraction of the top quark mass in Sect. 6.2 and the determination of ratios of cross-sections at different <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msqrt><mi>s</mi></msqrt></math> </ephtml> values in Sect. 6.3. The analyses were initially performed 'blind' by multiplying the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> values by an unknown, randomly chosen scale factor which was only removed after verifying that consistent results were obtained from the 2015 and 2016 datasets, and after finalising all systematic uncertainties and stability studies. As a validation of the analysis procedures, the yields of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>Z</mi><mo stretchy="false">→</mo><mi>e</mi><mi>e</mi></mrow></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>Z</mi><mo stretchy="false">→</mo><mi>μ</mi><mi>μ</mi></mrow></math> </ephtml> selections relative to the expectations from Powheg + Pythia8-based <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>Z</mi><mo stretchy="false">→</mo><mi>ℓ</mi><mi>ℓ</mi></mrow></math> </ephtml> simulation were also compared across all data-taking periods and trigger selections, and found to be compatible within the assigned systematic and very small statistical uncertainties.</p> <hd id="AN0144642803-17">Total and fiducial cross-section results</hd> <p>Table 5 shows the results for <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow><mi mathvariant="normal">fid</mi></msubsup></math> </ephtml> from the entire 2015–2016 dataset treated as a single sample, the 2015 and 2016 datasets separately, and the combination of 2015 and 2016 results. The latter was performed using the best linear unbiased estimator technique [[<reflink idref="bib90" id="ref119">90</reflink>]], taking into account correlations in the systematic uncertainties. The combination gives the smallest total uncertainty, 9% smaller than that from all data treated as one sample, and gives the final results:</p> <p> <ephtml> <math display="block" xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtable><mtr><mtd columnalign="right"><mrow><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub><mo>=</mo></mrow></mtd><mtd columnalign="left"><mrow><mrow /><mn>826.4</mn><mo>±</mo><mn>3.6</mn><mo>±</mo><mn>11.5</mn><mo>±</mo><mn>15.7</mn><mo>±</mo><mn>1.9</mn><mspace width="0.166667em" /><mi mathvariant="normal">pb</mi><mo>,</mo><mspace width="4pt" /><mi mathvariant="normal">and</mi></mrow></mtd></mtr><mtr><mtd columnalign="right"><mrow><mrow /><msubsup><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow><mi mathvariant="normal">fid</mi></msubsup><mo>=</mo></mrow></mtd><mtd columnalign="left"><mrow><mrow /><mn>14.07</mn><mo>±</mo><mn>0.06</mn><mo>±</mo><mn>0.18</mn><mo>±</mo><mn>0.27</mn><mo>±</mo><mn>0.03</mn><mspace width="0.166667em" /><mi mathvariant="normal">pb</mi><mo>,</mo></mrow></mtd></mtr></mtable></mrow></math> </ephtml> </p> <p>Graph</p> <p>where the four uncertainties are due to data statistics, experimental and theoretical systematic effects internal to the analysis, the knowledge of the integrated luminosity, and the knowledge of the LHC beam energy. The total relative uncertainties are 2.4% for both <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow><mi mathvariant="normal">fid</mi></msubsup></math> </ephtml> . The 2015 and 2016 datasets have relative weights of 0.49 and 0.51. The uncertainties due to the luminosity are only partially correlated and are similar in magnitude in both datasets, leading to approximately equal weights despite the much larger data sample from 2016. Other uncertainties are largely correlated between the two datasets, except for the statistical components of uncertainties estimated from data, such as the electron and muon identification efficiencies, and the misidentified-lepton background estimate. The <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi>χ</mi><mn>2</mn></msup></math> </ephtml> for the combination of 2015 and 2016 data is 0.23 for one degree of freedom, demonstrating good compatibility of the results. The values of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>ϵ</mi><mi>b</mi></msub></math> </ephtml> obtained in 2015 data and simulation are very similar, and 1.6% lower in 2016 data than simulation, well within the expected uncertainties in the modelling of <emph>b</emph>-tagging performance [[<reflink idref="bib70" id="ref120">70</reflink>]]. The result for <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> is reported for a fixed top quark mass of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>m</mi><mi>t</mi></msub><mo>=</mo><mn>172.5</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math> </ephtml> , and depends on the assumed value according to <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">(</mo><mn>1</mn><mo stretchy="false">/</mo><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub><mo stretchy="false">)</mo></mrow><mspace width="0.166667em" /><mi mathvariant="normal">d</mi><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub><mo stretchy="false">/</mo><mi mathvariant="normal">d</mi><msub><mi>m</mi><mi>t</mi></msub><mo>=</mo><mo>-</mo><mn>0.20</mn></mrow></math> </ephtml> %/ <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> . The <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>m</mi><mi>t</mi></msub></math> </ephtml> dependence of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow><mi mathvariant="normal">fid</mi></msubsup></math> </ephtml> is negligible. The fiducial cross-section was also corrected to remove the contribution of events with leptons from leptonic <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mi>τ</mi></math> </ephtml> decays as discussed in Sect. 4.2, giving a result of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msubsup><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo>,</mo><mi mathvariant="normal">no</mi><mo>-</mo><mi>τ</mi></mrow><mi mathvariant="normal">fid</mi></msubsup><mo>=</mo><mn>12.05</mn><mo>±</mo><mn>0.05</mn><mo>±</mo><mn>0.16</mn><mo>±</mo><mn>0.23</mn><mo>±</mo><mn>0.03</mn></mrow></math> </ephtml> pb.</p> <p>Measurements of the inclusive total ( <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> ) and fiducial ( <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow><mi mathvariant="normal">fid</mi></msubsup></math> </ephtml> ) <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> production cross-sections at <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> using the full dataset, the 2015 and 2016 datasets separately, and the combination of the 2015 and 2016 measurements. The fiducial cross-section requires an opposite-sign <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>e</mi><mi>μ</mi></mrow></math> </ephtml> pair, with both leptons having <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub><mo>></mo><mn>20</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mo stretchy="false">|</mo><mi>η</mi><mo stretchy="false">|</mo><mo><</mo><mn>2.5</mn></mrow></math> </ephtml> , as discussed in Sect. 4.1. The four uncertainties for each measurement correspond to the statistical, experimental and theoretical systematic, integrated luminosity, and beam energy uncertainties. The total uncertainty is given in parentheses after each result</p> <p> <ephtml> <table frame="hsides" rules="groups"><thead><tr><th align="left"><p>Dataset</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><msub xmlns=""><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math><inline-graphic href="10052_2020_7907_Article_IEq789.gif" /> (pb)</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup xmlns=""><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow><mi mathvariant="normal">fid</mi></msubsup></math><inline-graphic href="10052_2020_7907_Article_IEq790.gif" /> (pb)</p></th></tr></thead><tbody><tr><td align="left"><p>All data</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>830.7</mn><mo>±</mo><mn>2.2</mn><mo>±</mo><mn>11.6</mn><mo>±</mo><mn>18.4</mn><mo>±</mo><mn>1.9</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq791.gif" /> (22.0)</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>14.14</mn><mo>±</mo><mn>0.04</mn><mo>±</mo><mn>0.19</mn><mo>±</mo><mn>0.31</mn><mo>±</mo><mn>0.03</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq792.gif" /> (0.37)</p></td></tr><tr><td align="left"><p>2015 data</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>820.9</mn><mo>±</mo><mn>6.9</mn><mo>±</mo><mn>11.9</mn><mo>±</mo><mn>18.4</mn><mo>±</mo><mn>1.9</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq793.gif" /> (23.1)</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>13.98</mn><mo>±</mo><mn>0.12</mn><mo>±</mo><mn>0.19</mn><mo>±</mo><mn>0.31</mn><mo>±</mo><mn>0.03</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq794.gif" /> (0.39)</p></td></tr><tr><td align="left"><p>2016 data</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>831.8</mn><mo>±</mo><mn>2.3</mn><mo>±</mo><mn>11.6</mn><mo>±</mo><mn>19.5</mn><mo>±</mo><mn>1.9</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq795.gif" /> (22.9)</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>14.16</mn><mo>±</mo><mn>0.04</mn><mo>±</mo><mn>0.19</mn><mo>±</mo><mn>0.33</mn><mo>±</mo><mn>0.03</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq796.gif" /> (0.39)</p></td></tr><tr><td align="left"><p>Combination</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>826.4</mn><mo>±</mo><mn>3.6</mn><mo>±</mo><mn>11.5</mn><mo>±</mo><mn>15.7</mn><mo>±</mo><mn>1.9</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq797.gif" /> (19.9)</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>14.07</mn><mo>±</mo><mn>0.06</mn><mo>±</mo><mn>0.18</mn><mo>±</mo><mn>0.27</mn><mo>±</mo><mn>0.03</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq798.gif" /> (0.33)</p></td></tr></tbody></table> </ephtml> </p> <p>The breakdown of statistical and systematic uncertainties in the measurements is given in Table 4, which also shows the average uncertainty contributions to <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>ϵ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msub></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>C</mi><mi>b</mi></msub></math> </ephtml> , weighted as in the combination. The largest uncertainties come from the calibration of the integrated luminosity, followed by <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> modelling (generator, hadronisation, radiation and PDFs), background modelling (<emph>Wt</emph> single-top cross-section and misidentified leptons), and lepton identification efficiencies. The uncertainties due to <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> generator choices and PDFs are smaller for <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow><mi mathvariant="normal">fid</mi></msubsup></math> </ephtml> than for <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> , but are offset by a larger uncertainty due to <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> hadronisation, such that the total uncertainties in the two measurements are very similar.</p> <p>The results are stable within the statistical uncertainties when increasing the minimum jet <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> requirement from the nominal value of 25 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> up to 75 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> , where the tagging correlations become much stronger ( <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>C</mi><mi>b</mi></msub><mo>=</mo><mn>1.16</mn></mrow></math> </ephtml> ). The results are also stable when tightening the jet selection to <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mo stretchy="false">|</mo><mi>η</mi><mo stretchy="false">|</mo><mo><</mo><mn>1.0</mn></mrow></math> </ephtml> and changing the <emph>b</emph>-tagging selection to use the 60% or 77% efficiency working points. However, a significant trend was found when tightening the lepton <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> requirement from the nominal <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub><mo>></mo><mn>20</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math> </ephtml> in several steps up to <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub><mo>></mo><mn>55</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math> </ephtml> , where <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>ϵ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msub></math> </ephtml> is reduced by a factor 4.4 and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> changes by <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mo>-</mo><mn>3.9</mn><mo>±</mo><mn>0.7</mn></mrow></math> </ephtml> %, the uncertainty corresponding to the uncorrelated statistical component only. This is caused by the lepton <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> spectrum in data being significantly softer than that in the baseline Powheg + Pythia8 simulation (see Fig. 1c, e, and Fig. 12a below). As discussed in Sect. 7.2 and shown in Fig. 16, the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>ℓ</mi></msubsup></math> </ephtml> distribution is better described by the alternative aMC@NLO + Pythia8 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> sample, or by reweighting the baseline Powheg + Pythia8 sample to better describe the measured top quark <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> spectrum [[<reflink idref="bib92" id="ref121">92</reflink>]]. Using either of these <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> samples to calculate <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>ϵ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msub></math> </ephtml> increases the measured <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> with a lepton <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub><mo>></mo><mn>20</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math> </ephtml> requirement by about 0.5%, and greatly improves the stability of the result against changes in the lepton <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> requirement. Since this change is similar to the already assigned <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> modelling uncertainties (in particular from the aMC@NLO vs Powheg comparison), no additional uncertainty was included.</p> <p>The inclusive cross-section result, together with previous measurements at <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>7</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>8</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> [[<reflink idref="bib7" id="ref122">7</reflink>]], is compared in Fig. 8 with the NNLO+NNLL QCD prediction described in Sect. 1. The measurement agrees with the predictions using the CT10, MSTW2008 and NNPDF2.3 PDF sets combined with the PDF4LHC prescription. It is significantly more precise than this prediction, demonstrating the power of the measurement to constrain the gluon PDF at high Bjorken-<emph>x</emph>. The lower ratio panel compares the measurements to predictions using the CT14 [[<reflink idref="bib74" id="ref123">74</reflink>]] and NNPDF3.1_notop [[<reflink idref="bib93" id="ref124">93</reflink>]] NNLO PDF sets, two recent PDF sets which do not use any <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> data in their fits. The NNPDF3.1_notop PDF set does not include any variations of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>α</mi><mi mathvariant="normal">S</mi></msub></math> </ephtml> from the nominal value of 0.118, so the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>α</mi><mi mathvariant="normal">S</mi></msub></math> </ephtml> uncertainty obtained from an <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>α</mi><mi mathvariant="normal">S</mi></msub></math> </ephtml> variation of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mo>±</mo><mn>0.0012</mn></mrow></math> </ephtml> with the standard NNPDF3.1 PDF set was added in quadrature to the PDF-alone uncertainty calculated with NNPDF3.1_notop. The <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> measurement is also in good agreement with the predictions from these PDF sets.</p> <p>The result is also consistent with, and supersedes, the previous ATLAS measurement using the same technique applied to 2015 data alone, which had an uncertainty of 4.4% [[<reflink idref="bib9" id="ref125">9</reflink>]]. The smaller uncertainty of 2.4% in the updated analysis results from improvements in the modelling of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> production (including tuning to <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> data at <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> ), more precise calibration of the integrated luminosity and of the LHC beam energy, and better understanding of the lepton identification efficiencies and energy scales, as well as the larger data sample. The new result is also consistent with results from CMS in the dilepton [[<reflink idref="bib13" id="ref126">13</reflink>]] and lepton+jets [[<reflink idref="bib12" id="ref127">12</reflink>]] final states, but again has higher precision.</p> <p>Graph: Fig. 8 The upper plot shows the inclusive tt¯ cross-section σtt¯ as a function of centre-of-mass energy s, comparing ATLAS results from the eμ plus b-tagged jets final state at s=7, 8 and 13 Te with NNLO+NNLL theoretical predictions [[<reflink idref="bib5" id="ref128">5</reflink>]] calculated using Top++ [[<reflink idref="bib14" id="ref129">14</reflink>]] using the PDF4LHC prescription for PDF and αS uncertainties [[<reflink idref="bib15" id="ref130">15</reflink>]], and mt=172.5Ge. The middle plot shows the ratios of the measurements and predictions to the central value of the prediction using PDF4LHC. The total uncertainties when using the individual NNPDF2.3, MSTW and CT10 PDFs are shown as overlapping hatched or coloured bands, and the dotted lines show the QCD scale uncertainties alone. The lower plot shows the ratios of the measurements and predictions from the CT14 and NNPDF3.1_notop PDFs to the central value from CT14. The s=7 and 8 Te results are taken from Ref. [[<reflink idref="bib7" id="ref131">7</reflink>]], with the LHC beam energy uncertainties reduced according to Ref. [[<reflink idref="bib88" id="ref132">88</reflink>]]</p> <hd id="AN0144642803-18">Extraction of the top quark pole mass</hd> <p>The strong dependence of the inclusive <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> cross-section prediction on the top quark pole mass <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>m</mi><mi>t</mi><mi mathvariant="normal">pole</mi></msubsup></math> </ephtml> can be exploited to interpret precise measurements of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> as measurements of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>m</mi><mi>t</mi><mi mathvariant="normal">pole</mi></msubsup></math> </ephtml> , as discussed in Sect. 1. The ATLAS <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>7</mn></mrow></math> </ephtml> and 8 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> measurements in the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>e</mi><mi>μ</mi></mrow></math> </ephtml> channel were interpreted in this way, giving a combined value of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msubsup><mi>m</mi><mi>t</mi><mi mathvariant="normal">pole</mi></msubsup><mo>=</mo><mn>172</mn><mo>.</mo><msubsup><mn>9</mn><mrow><mo>-</mo><mn>2.6</mn></mrow><mrow><mo>+</mo><mn>2.5</mn></mrow></msubsup><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math> </ephtml> [[<reflink idref="bib7" id="ref133">7</reflink>]], and similar measurements have been performed by CMS at <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>7</mn></mrow></math> </ephtml> , 8 and 13 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> [[<reflink idref="bib10" id="ref134">10</reflink>], [<reflink idref="bib12" id="ref135">12</reflink>]], as well as by D0 at the Tevatron <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mover accent="true"><mrow><mi>p</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mi>p</mi></mrow></math> </ephtml> collider [[<reflink idref="bib94" id="ref136">94</reflink>]].</p> <p>The NNLO+NNLL prediction for <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> as a function of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>m</mi><mi>t</mi><mi mathvariant="normal">pole</mi></msubsup></math> </ephtml> at <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> was calculated using Top++ [[<reflink idref="bib14" id="ref137">14</reflink>]] and the CT14 NNLO PDF set [[<reflink idref="bib74" id="ref138">74</reflink>]] with uncertainties scaled to 68% confidence levels and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>α</mi><mi mathvariant="normal">S</mi></msub><mo>=</mo><mn>0.1180</mn><mo>±</mo><mn>0.0012</mn></mrow></math> </ephtml> . CT14 was chosen as a recent PDF set which does not use any <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> cross-section data as input. The resulting dependence was parameterised using the functional form proposed in Ref. [[<reflink idref="bib5" id="ref139">5</reflink>]]:</p> <p> <ephtml> <math display="block" xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtable><mtr><mtd columnalign="right"><mrow><msubsup><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow><mi mathvariant="normal">theo</mi></msubsup><mrow><mo stretchy="false">(</mo><msubsup><mi>m</mi><mi>t</mi><mi mathvariant="normal">pole</mi></msubsup><mo stretchy="false">)</mo></mrow><mo>=</mo><mi>σ</mi><mrow><mo stretchy="false">(</mo><msubsup><mi>m</mi><mi>t</mi><mi mathvariant="normal">ref</mi></msubsup><mo stretchy="false">)</mo></mrow><msup><mfenced close=")" open="(" separators=""><mfrac><msubsup><mi>m</mi><mi>t</mi><mi mathvariant="normal">ref</mi></msubsup><msubsup><mi>m</mi><mi>t</mi><mi mathvariant="normal">pole</mi></msubsup></mfrac></mfenced><mn>4</mn></msup><mrow><mo stretchy="false">(</mo><mn>1</mn><mo>+</mo><msub><mi>a</mi><mn>1</mn></msub><mi>x</mi><mo>+</mo><msub><mi>a</mi><mn>2</mn></msub><msup><mi>x</mi><mn>2</mn></msup><mo stretchy="false">)</mo></mrow><mo>.</mo></mrow></mtd></mtr></mtable></mrow></math> </ephtml> </p> <p>Graph</p> <p>Here, <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>x</mi><mo>=</mo><mrow><mo stretchy="false">(</mo><msubsup><mi>m</mi><mi>t</mi><mi mathvariant="normal">pole</mi></msubsup><mo>-</mo><msubsup><mi>m</mi><mi>t</mi><mi mathvariant="normal">ref</mi></msubsup><mo stretchy="false">)</mo></mrow><mo stretchy="false">/</mo><msubsup><mi>m</mi><mi>t</mi><mi mathvariant="normal">ref</mi></msubsup></mrow></math> </ephtml> , the constant <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msubsup><mi>m</mi><mi>t</mi><mi mathvariant="normal">ref</mi></msubsup><mo>=</mo><mn>172.5</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math> </ephtml> , and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>σ</mi><mo stretchy="false">(</mo><msubsup><mi>m</mi><mi>t</mi><mi mathvariant="normal">ref</mi></msubsup><mo stretchy="false">)</mo></mrow></math> </ephtml> , <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>a</mi><mn>1</mn></msub></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>a</mi><mn>2</mn></msub></math> </ephtml> are free parameters. The resulting function is shown in Fig. 9. The measurement of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> given in Sect. 6.1 is also shown, with its small dependence on <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>m</mi><mi>t</mi></msub></math> </ephtml> due to variations of the experimental acceptance and <emph>Wt</emph> background discussed in Sect. 5.1. These variations were studied using <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> and <emph>Wt</emph> simulation samples with several values of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>m</mi><mi>t</mi></msub></math> </ephtml> , and the corresponding dependencies of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>ϵ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msub></math> </ephtml> , <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>N</mi><mn>1</mn><mi mathvariant="normal">bkg</mi></msubsup></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>N</mi><mn>2</mn><mi mathvariant="normal">bkg</mi></msubsup></math> </ephtml> on <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>m</mi><mi>t</mi></msub></math> </ephtml> were parameterised with second-order polynomials. The mass parameter used to characterise the dependence of the measured <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> on <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>m</mi><mi>t</mi></msub></math> </ephtml> represents the top quark mass used in the Monte Carlo event generators rather than <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>m</mi><mi>t</mi><mi mathvariant="normal">pole</mi></msubsup></math> </ephtml> , but since the dependence of the measured <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> on <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>m</mi><mi>t</mi></msub></math> </ephtml> is small, this approximation causes negligible bias if <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>m</mi><mi>t</mi></msub></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>m</mi><mi>t</mi><mi mathvariant="normal">pole</mi></msubsup></math> </ephtml> differ by only a few <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> . Under these conditions, the intersection of the theoretical and experimental curves shown in Fig. 9 gives an unambiguous extraction of the top quark pole mass.</p> <p>Graph: Fig. 9 Predicted inclusive tt¯ cross-section at s=13Te as a function of the top quark pole mass mtpole, for the CT14 PDF set. The cyan band indicates the total uncertainty in the prediction from PDF+αS and QCD scale uncertainties. The experimental measurement with its uncertainty and dependence on the assumed value of mt through acceptance and background corrections is shown by the black points with error bars</p> <p>The mass extraction was performed by maximising the following Bayesian likelihood as a function of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>m</mi><mi>t</mi><mi mathvariant="normal">pole</mi></msubsup></math> </ephtml> :</p> <p>7 <ephtml> <math display="block" xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtable><mtr><mtd columnalign="right"><mrow><mi mathvariant="script">L</mi><mo stretchy="false">(</mo><msubsup><mi>m</mi><mi>t</mi><mi mathvariant="normal">pole</mi></msubsup><mo stretchy="false">)</mo><mo>=</mo></mrow></mtd><mtd columnalign="left"><mrow><mrow /><mo>∫</mo><mi>G</mi><mo stretchy="false">(</mo><msubsup><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow><mo>′</mo></msubsup><mspace width="0.166667em" /><mo stretchy="false">|</mo><mspace width="0.166667em" /><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub><mrow><mo stretchy="false">(</mo><msubsup><mi>m</mi><mi>t</mi><mi mathvariant="normal">pole</mi></msubsup><mo stretchy="false">)</mo></mrow><mo>,</mo><msub><mi>s</mi><mi mathvariant="normal">exp</mi></msub><mo stretchy="false">)</mo></mrow></mtd></mtr><mtr><mtd columnalign="right"><mrow /></mtd><mtd columnalign="left"><mrow><mo>·</mo><mspace width="0.166667em" /><mi>G</mi><mrow><mo stretchy="false">(</mo><msubsup><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow><mo>′</mo></msubsup><mspace width="0.166667em" /><mo stretchy="false">|</mo><mspace width="0.166667em" /><msubsup><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow><mi mathvariant="normal">theo</mi></msubsup><mrow><mo stretchy="false">(</mo><msubsup><mi>m</mi><mi>t</mi><mi mathvariant="normal">pole</mi></msubsup><mo stretchy="false">)</mo></mrow><mo>,</mo><msubsup><mi>s</mi><mi mathvariant="normal">theo</mi><mo>±</mo></msubsup><mspace width="0.166667em" /><mo stretchy="false">)</mo></mrow><mspace width="4pt" /><mi mathvariant="normal">d</mi><msubsup><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow><mo>′</mo></msubsup><mo>,</mo></mrow></mtd></mtr></mtable></mrow></math> </ephtml></p> <p>Graph</p> <p>where <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>G</mi><mo stretchy="false">(</mo><mi>x</mi><mspace width="0.166667em" /><mo stretchy="false">|</mo><mspace width="0.166667em" /><mi>μ</mi><mo>,</mo><mi>s</mi><mo stretchy="false">)</mo></mrow></math> </ephtml> represents a Gaussian probability density in the variable <emph>x</emph> with mean <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mi>μ</mi></math> </ephtml> and standard deviation <emph>s</emph>. The first Gaussian term in the integral represents the experimental measurement <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> with its dependence on <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>m</mi><mi>t</mi><mi mathvariant="normal">pole</mi></msubsup></math> </ephtml> and uncertainty <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>s</mi><mi mathvariant="normal">exp</mi></msub></math> </ephtml> , and the second term represents the theoretical prediction <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow><mi mathvariant="normal">theo</mi></msubsup></math> </ephtml> with its asymmetric uncertainty <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>s</mi><mi mathvariant="normal">theo</mi><mo>±</mo></msubsup></math> </ephtml> obtained from the quadrature sum of the combined PDF plus <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>α</mi><mi mathvariant="normal">S</mi></msub></math> </ephtml> uncertainty, and the QCD scale uncertainty, each evaluated as described in Sect. 1. The likelihood in Eq. (<reflink idref="bib7" id="ref140">7</reflink>) was maximised to obtain <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>m</mi><mi>t</mi><mi mathvariant="normal">pole</mi></msubsup></math> </ephtml> when using the CT14 NNLO PDF set to calculate <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow><mi mathvariant="normal">theo</mi></msubsup></math> </ephtml> , and also when using the NNPDF3.1_notop NNLO PDF set, with <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>α</mi><mi mathvariant="normal">S</mi></msub></math> </ephtml> uncertainties inferred from NNPDF3.1 as discussed in Sect. 6.1. Results were also obtained using the individual CT10, MSTW and NNPDF2.3 NNLO PDF sets to calculate <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow><mi mathvariant="normal">theo</mi></msubsup></math> </ephtml> , for comparison with the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>7</mn></mrow></math> </ephtml> and 8 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> results. The MMHT and NNPDF3.0 PDF sets were not considered, as they include <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> cross-section data in order to constrain the gluon PDF, and hence cannot also be used to determine <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>m</mi><mi>t</mi><mi mathvariant="normal">pole</mi></msubsup></math> </ephtml> without introducing a circular dependence [[<reflink idref="bib95" id="ref141">95</reflink>]]. In each case, the value of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> was recalculated using the corresponding NLO PDF set to calculate the value of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>ϵ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msub></math> </ephtml> . The results from each PDF set are shown in Table 6, together with the result using the PDF4LHC prescription to combine the CT10, MSTW and NNPDF2.3 results, keeping the CT10 central value but enlarging the uncertainty to cover the envelope of the positive and negative uncertainties of each individual PDF set. The NNPDF3.1_notop PDF set gives the smallest uncertainty of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mo>±</mo><mn>1.7</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math> </ephtml> , demonstrating the power of recent improvements in the gluon PDF determination to reduce the uncertainty on <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>m</mi><mi>t</mi><mi mathvariant="normal">pole</mi></msubsup></math> </ephtml> . However, given the approximate procedure used to evaluate the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>α</mi><mi mathvariant="normal">S</mi></msub></math> </ephtml> uncertainty for this PDF set, the CT14 PDF set was chosen for the baseline result.</p> <p>Top quark pole mass results for various NNLO PDF sets, derived from the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> cross-section measurement at <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> . The uncertainties include PDF+ <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>α</mi><mi mathvariant="normal">S</mi></msub></math> </ephtml> , QCD scale and experimental sources. The PDF4LHC result spans the uncertainties of the CT10, MSTW and NNPDF2.3 PDF sets</p> <p> <ephtml> <table frame="hsides" rules="groups"><thead><tr><th align="left"><p>PDF set</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup xmlns=""><mi>m</mi><mi>t</mi><mi mathvariant="normal">pole</mi></msubsup></math><inline-graphic href="10052_2020_7907_Article_IEq922.gif" /> (GeV)</p></th></tr></thead><tbody><tr><td align="left"><p>CT14</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>173</mn><mo>.</mo><msubsup><mn>1</mn><mrow><mo>-</mo><mn>2.1</mn></mrow><mrow><mo>+</mo><mn>2.0</mn></mrow></msubsup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq923.gif" /></p></td></tr><tr><td align="left"><p>NNPDF3.1_notop</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>172</mn><mo>.</mo><msubsup><mn>9</mn><mrow><mo>-</mo><mn>1.7</mn></mrow><mrow><mo>+</mo><mn>1.7</mn></mrow></msubsup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq924.gif" /></p></td></tr><tr><td align="left"><p>CT10</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>172</mn><mo>.</mo><msubsup><mn>1</mn><mrow><mo>-</mo><mn>2.0</mn></mrow><mrow><mo>+</mo><mn>2.0</mn></mrow></msubsup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq925.gif" /></p></td></tr><tr><td align="left"><p>MSTW</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>172</mn><mo>.</mo><msubsup><mn>3</mn><mrow><mo>-</mo><mn>2.1</mn></mrow><mrow><mo>+</mo><mn>2.0</mn></mrow></msubsup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq926.gif" /></p></td></tr><tr><td align="left"><p>NNPDF2.3</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>173</mn><mo>.</mo><msubsup><mn>4</mn><mrow><mo>-</mo><mn>1.9</mn></mrow><mrow><mo>+</mo><mn>1.9</mn></mrow></msubsup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq927.gif" /></p></td></tr><tr><td align="left"><p>PDF4LHC</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>172</mn><mo>.</mo><msubsup><mn>1</mn><mrow><mo>-</mo><mn>2.0</mn></mrow><mrow><mo>+</mo><mn>3.1</mn></mrow></msubsup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq928.gif" /></p></td></tr></tbody></table> </ephtml> </p> <p>Table 7 shows the breakdown of uncertainties in <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>m</mi><mi>t</mi><mi mathvariant="normal">pole</mi></msubsup></math> </ephtml> calculated using the CT14 PDF set, which are dominated by uncertainties in <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow><mi mathvariant="normal">theo</mi></msubsup></math> </ephtml> through PDF+ <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>α</mi><mi mathvariant="normal">S</mi></msub></math> </ephtml> and QCD scale variations. Improving the experimental measurement of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> further would therefore have little effect on the determination of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>m</mi><mi>t</mi><mi mathvariant="normal">pole</mi></msubsup></math> </ephtml> via this method. The result is compatible with other measurements of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>m</mi><mi>t</mi><mi mathvariant="normal">pole</mi></msubsup></math> </ephtml> via lepton differential distributions [[<reflink idref="bib29" id="ref142">29</reflink>]], and via the reconstruction of top quark differential distributions in inclusive <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> [[<reflink idref="bib96" id="ref143">96</reflink>]] and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> +jet [[<reflink idref="bib97" id="ref144">97</reflink>]] events, as well as previous measurements using the total <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> cross-section [[<reflink idref="bib7" id="ref145">7</reflink>], [<reflink idref="bib10" id="ref146">10</reflink>], [<reflink idref="bib12" id="ref147">12</reflink>], [<reflink idref="bib94" id="ref148">94</reflink>]]. It is also consistent with the Particle Data Group average of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msubsup><mi>m</mi><mi>t</mi><mi mathvariant="normal">pole</mi></msubsup><mo>=</mo><mn>173.1</mn><mo>±</mo><mn>0.9</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math> </ephtml> [[<reflink idref="bib99" id="ref149">99</reflink>]] from a subset of these measurements. The result using the CT14 PDF improves upon the previous ATLAS result from <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>7</mn></mrow></math> </ephtml> and 8 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> data using the CT10, MSTW and NNPDF2.3 PDFs combined with the PDF4LHC prescription [[<reflink idref="bib7" id="ref150">7</reflink>]]. However, using the PDF4LHC prescription with the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> data gives a larger uncertainty of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msubsup><mrow /><mrow><mo>-</mo><mn>2.0</mn></mrow><mrow><mo>+</mo><mn>3.1</mn></mrow></msubsup><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math> </ephtml> , as the prediction of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> from NNPDF2.3 starts to diverge from that of CT10 and MSTW at higher <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msqrt><mi>s</mi></msqrt></math> </ephtml> (see Fig. 8), leading to a larger spread in the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>m</mi><mi>t</mi></msub></math> </ephtml> values from the different PDF sets.</p> <p>Uncertainties in the top quark pole mass extracted from the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> production cross-section measurement at <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> , using the CT14 PDF set</p> <p> <ephtml> <table frame="hsides" rules="groups"><thead><tr><th align="left"><p>Uncertainty source</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi mathvariant="normal">Δ</mi><msubsup><mi>m</mi><mi>t</mi><mi mathvariant="normal">pole</mi></msubsup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq950.gif" /> (GeV)</p></th></tr></thead><tbody><tr><td align="left"><p>Data statistics</p></td><td align="left"><p>0.2</p></td></tr><tr><td align="left"><p>Analysis systematics</p></td><td align="left"><p>0.6</p></td></tr><tr><td align="left"><p>Integrated luminosity</p></td><td align="left"><p>0.8</p></td></tr><tr><td align="left"><p>Beam energy</p></td><td align="left"><p>0.1</p></td></tr><tr><td align="left"><p>PDF+<math xmlns="http://www.w3.org/1998/Math/MathML"><msub xmlns=""><mi>α</mi><mi mathvariant="normal">S</mi></msub></math><inline-graphic href="10052_2020_7907_Article_IEq951.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup xmlns=""><mrow /><mrow><mo>-</mo><mn>1.4</mn></mrow><mrow><mo>+</mo><mn>1.5</mn></mrow></msubsup></math><inline-graphic href="10052_2020_7907_Article_IEq952.gif" /></p></td></tr><tr><td align="left"><p>QCD scales</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup xmlns=""><mrow /><mrow><mo>-</mo><mn>1.5</mn></mrow><mrow><mo>+</mo><mn>1.0</mn></mrow></msubsup></math><inline-graphic href="10052_2020_7907_Article_IEq953.gif" /></p></td></tr><tr><td align="left"><p>Total uncertainty</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup xmlns=""><mrow /><mrow><mo>-</mo><mn>2.1</mn></mrow><mrow><mo>+</mo><mn>2.0</mn></mrow></msubsup></math><inline-graphic href="10052_2020_7907_Article_IEq954.gif" /></p></td></tr></tbody></table> </ephtml> </p> <hd id="AN0144642803-19">tt¯ and tt¯/Z cross-section ratios at different energies</hd> <p>The ratios <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>R</mi><mrow><mn>13</mn><mo stretchy="false">/</mo><mn>7</mn></mrow><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msubsup></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>R</mi><mrow><mn>13</mn><mo stretchy="false">/</mo><mn>8</mn></mrow><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msubsup></math> </ephtml> were calculated using the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> result discussed above and the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>7</mn></mrow></math> </ephtml> and 8 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> results from Refs. [[<reflink idref="bib7" id="ref151">7</reflink>]], corrected to reduce the LHC beam energy uncertainty to 0.1% [[<reflink idref="bib88" id="ref152">88</reflink>]]. The <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> values and uncertainties are summarised in Table 8; the largest systematic uncertainties come in all cases from <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> modelling and the knowledge of the integrated luminosity. As the nominal <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> simulation sample used at <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>7</mn></mrow></math> </ephtml> and 8 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> was Powheg + Pythia6 with the CT10 PDFs, the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> result was rederived using a similar <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> sample to calculate <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>ϵ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msub></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>C</mi><mi>b</mi></msub></math> </ephtml> , increasing the 13 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> value by 0.46%. PDF uncertainties were evaluated for each of the error sets or replicas of the CT10, MSTW and NNPDF2.3 PDF sets, considering the effect of each individual variation to be correlated between the numerator and denominator of the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> ratio. Significant cancellations occur, leading to PDF uncertainties of about 0.5% in each ratio, significantly smaller than the 1% uncertainties for the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>7</mn></mrow></math> </ephtml> and 8 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> measurements. The parton-shower radiation uncertainties were similarly evaluated using Powheg + Pythia6 samples with more and less parton-shower radiation in all datasets, giving residual uncertainties of around 0.4% in the ratios. Other <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> modelling uncertainties due to the choice of NLO generator and hadronisation model were conservatively taken to be uncorrelated, due to the different alternative generators used in the measurements. The uncertainties due to the <emph>Wt</emph> background cross-section and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo stretchy="false">/</mo><mi>W</mi><mi>t</mi></mrow></math> </ephtml> interference were assessed in the same way at all <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msqrt><mi>s</mi></msqrt></math> </ephtml> values and considered correlated. Lepton, jet and <emph>b</emph>-tagging uncertainties were mainly considered uncorrelated, due to the changes in detector configuration and lepton identification algorithms between measurements. The integrated luminosity measurements were based on different primary detectors at 7–8 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> and 13 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> , and the luminosity scale was calibrated using individual beam-separation scans in each dataset [[<reflink idref="bib86" id="ref153">86</reflink>], [<reflink idref="bib100" id="ref154">100</reflink>]] with only a fraction of the uncertainties being correlated. The total luminosity uncertainties were therefore conservatively taken to be uncorrelated in the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> ratio measurements. The beam energy uncertainties are correlated between <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msqrt><mi>s</mi></msqrt></math> </ephtml> values, but the varying dependence of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> on <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msqrt><mi>s</mi></msqrt></math> </ephtml> (see Fig. 8) leads to a small ( <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mo><</mo><mn>0.1</mn></mrow></math> </ephtml> %) residual uncertainty on the ratios.</p> <p>Input inclusive <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> and fiducial <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>Z</mi><mo stretchy="false">→</mo><mi>e</mi><mi>e</mi><mo stretchy="false">/</mo><mi>μ</mi><mi>μ</mi></mrow></math> </ephtml> cross-sections used in the calculations of the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo stretchy="false">/</mo><mi>Z</mi></mrow></math> </ephtml> cross-section ratios and double ratios shown in Tables 9 and 10. The three uncertainties in each cross-section are due to data statistics, experimental and theoretical systematic effects (including the LHC beam energy uncertainties) and knowledge of the integrated luminosities of the data samples. For <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> , the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> cross-section labelled (<emph>a</emph>) uses 2015 data only and is used for the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo stretchy="false">/</mo><mi>Z</mi></mrow></math> </ephtml> ratio <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>R</mi><mn>13</mn><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo stretchy="false">/</mo><mi>Z</mi></mrow></msubsup></math> </ephtml> and the double ratios <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>R</mi><mrow><mn>13</mn><mo stretchy="false">/</mo><mn>7</mn></mrow><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo stretchy="false">/</mo><mi>Z</mi></mrow></msubsup></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>R</mi><mrow><mn>13</mn><mo stretchy="false">/</mo><mn>8</mn></mrow><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo stretchy="false">/</mo><mi>Z</mi></mrow></msubsup></math> </ephtml> , whilst the cross-section labelled (<emph>b</emph>) uses the combination of 2015 and 2016 data, and is used for the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> cross-section ratios <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>R</mi><mrow><mn>13</mn><mo stretchy="false">/</mo><mn>7</mn></mrow><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msubsup></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>R</mi><mrow><mn>13</mn><mo stretchy="false">/</mo><mn>8</mn></mrow><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msubsup></math> </ephtml> . Both <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> cross-sections have been calculated using a Powheg + Pythia6 sample to derive the efficiencies (see text)</p> <p> <ephtml> <table frame="hsides" rules="groups"><thead><tr><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><msqrt xmlns=""><mi>s</mi></msqrt></math><inline-graphic href="10052_2020_7907_Article_IEq1005.gif" /> (<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1006.gif" />)</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><msub xmlns=""><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math><inline-graphic href="10052_2020_7907_Article_IEq1007.gif" />(pb)</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup xmlns=""><mi>σ</mi><mrow><mi>Z</mi><mo stretchy="false">→</mo><mi>e</mi><mi>e</mi></mrow><mi mathvariant="normal">fid</mi></msubsup></math><inline-graphic href="10052_2020_7907_Article_IEq1008.gif" /> (pb)</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup xmlns=""><mi>σ</mi><mrow><mi>Z</mi><mo stretchy="false">→</mo><mi>μ</mi><mi>μ</mi></mrow><mi mathvariant="normal">fid</mi></msubsup></math><inline-graphic href="10052_2020_7907_Article_IEq1009.gif" /> (pb)</p></th></tr></thead><tbody><tr><td align="left"><p>7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>182.9</mn><mo>±</mo><mn>3.1</mn><mo>±</mo><mn>4.2</mn><mo>±</mo><mn>3.6</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1010.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>451.2</mn><mo>±</mo><mn>0.5</mn><mo>±</mo><mn>1.7</mn><mo>±</mo><mn>8.1</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1011.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>450.0</mn><mo>±</mo><mn>0.4</mn><mo>±</mo><mn>2.0</mn><mo>±</mo><mn>8.1</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1012.gif" /></p></td></tr><tr><td align="left"><p>8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>242.9</mn><mo>±</mo><mn>1.7</mn><mo>±</mo><mn>5.5</mn><mo>±</mo><mn>5.1</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1013.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>507.0</mn><mo>±</mo><mn>0.2</mn><mo>±</mo><mn>4.3</mn><mo>±</mo><mn>9.6</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1014.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>504.7</mn><mo>±</mo><mn>0.2</mn><mo>±</mo><mn>3.6</mn><mo>±</mo><mn>9.6</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1015.gif" /></p></td></tr><tr><td align="left" rowspan="2"><p>13</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>824.7</mn><mo>±</mo><mn>6.9</mn><mo>±</mo><mn>12.1</mn><mo>±</mo><mn>18</mn><mo>.</mo><msup><mn>4</mn><mrow><mo stretchy="false">(</mo><mi>a</mi><mo stretchy="false">)</mo></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1016.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>778.3</mn><mo>±</mo><mn>0.7</mn><mo>±</mo><mn>4.1</mn><mo>±</mo><mn>15.9</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1017.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>774.4</mn><mo>±</mo><mn>0.7</mn><mo>±</mo><mn>6.3</mn><mo>±</mo><mn>15.8</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1018.gif" /></p></td></tr><tr><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>830.2</mn><mo>±</mo><mn>3.6</mn><mo>±</mo><mn>11.7</mn><mo>±</mo><mn>15</mn><mo>.</mo><msup><mn>7</mn><mrow><mo stretchy="false">(</mo><mi>b</mi><mo stretchy="false">)</mo></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1019.gif" /></p></td><td align="left" /><td align="left" /></tr></tbody></table> </ephtml> </p> <p>The resulting cross-section ratios are shown in Table 9, together with the NNLO+NNLL predictions calculated using Top++ as described in Sect. 1, with the uncertainties from the CT10, MSTW and NNPDF2.3 PDFs combined according to the PDF4LHC prescription. The total uncertainties in the measurements are 3.9% for <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>R</mi><mrow><mn>13</mn><mo stretchy="false">/</mo><mn>7</mn></mrow><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msubsup></math> </ephtml> and 3.6% for <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>R</mi><mrow><mn>13</mn><mo stretchy="false">/</mo><mn>8</mn></mrow><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msubsup></math> </ephtml> , improving on the uncertainties of 4.9% and 4.7% obtained using the 2015 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> dataset alone in Ref. [[<reflink idref="bib27" id="ref155">27</reflink>]]. Figure 10 compares the measurements with the predictions using the CT10, MSTW and NNPDF2.3 PDF sets, as well as the more recent CT14 [[<reflink idref="bib74" id="ref156">74</reflink>]], ABM12LHC [[<reflink idref="bib102" id="ref157">102</reflink>]], ABMP16 [[<reflink idref="bib103" id="ref158">103</reflink>]], ATLAS-epWZ12 [[<reflink idref="bib104" id="ref159">104</reflink>]], HERAPDF2.0 [[<reflink idref="bib105" id="ref160">105</reflink>]], MMHT14 [[<reflink idref="bib77" id="ref161">77</reflink>]] and NNPDF3.0 [[<reflink idref="bib44" id="ref162">44</reflink>]] PDF sets, some of which include some LHC data (including <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> cross-section measurements in the cases of ABM12LHC, ABMP16, MMHT and NNPDF3.0). The ratio <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>R</mi><mrow><mn>13</mn><mo stretchy="false">/</mo><mn>7</mn></mrow><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msubsup></math> </ephtml> is lower than all the predictions, and the ratio <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>R</mi><mrow><mn>13</mn><mo stretchy="false">/</mo><mn>8</mn></mrow><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msubsup></math> </ephtml> higher than all the predictions except ABM12LHC. However, both ratios are compatible with all the predictions except ABM12LHC within two standard deviations. Some of these results are also reflected in Fig. 8. The behaviour of ABM12LHC is attributed to the lower gluon density at high Bjorken-<emph>x</emph> compared to the other considered PDF sets, which leads to a larger relative increase in the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> cross-section as a function of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msqrt><mi>s</mi></msqrt></math> </ephtml> . This behaviour is less apparent in the more recent ABMP16 PDF set, which includes more precise constraints from LHC top quark measurements. The current experimental uncertainties, dominated by the luminosity uncertainties which do not cancel in the ratios, do not allow the predictions using the other PDFs to be distinguished.</p> <p>Ratios of inclusive <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> production cross-sections measured at <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></mrow></math> </ephtml> , 7 and 8 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> , together with the corresponding NNLO+NNLL predictions using Top++ [[<reflink idref="bib14" id="ref163">14</reflink>]] with the PDF4LHC prescription for PDF and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>α</mi><mi mathvariant="normal">S</mi></msub></math> </ephtml> uncertainties [[<reflink idref="bib15" id="ref164">15</reflink>]]. The three uncertainties in the measured ratios are due to data statistics, experimental and theoretical systematic effects (including the LHC beam energy uncertainties) and knowledge of the integrated luminosities of the data samples. The ratio of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>8</mn></mrow></math> </ephtml> and 7 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> results is taken from Ref. [[<reflink idref="bib7" id="ref165">7</reflink>]]. The total uncertainty is given in parentheses after each result</p> <p> <ephtml> <table frame="hsides" rules="groups"><thead><tr><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><msqrt xmlns=""><mi>s</mi></msqrt></math><inline-graphic href="10052_2020_7907_Article_IEq1035.gif" /> values (<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1036.gif" />)</p></th><th align="left"><p>Measured cross-section ratio</p></th><th align="left"><p>NNLO+NNLL prediction</p></th></tr></thead><tbody><tr><td align="left"><p>13/7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4.54</mn><mo>±</mo><mn>0.08</mn><mo>±</mo><mn>0.10</mn><mo>±</mo><mn>0.12</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1037.gif" /> (0.18)</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4.69</mn><mo>±</mo><mn>0.16</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1038.gif" /></p></td></tr><tr><td align="left"><p>13/8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3.42</mn><mo>±</mo><mn>0.03</mn><mo>±</mo><mn>0.07</mn><mo>±</mo><mn>0.10</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1039.gif" /> (0.12)</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3.28</mn><mo>±</mo><mn>0.08</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1040.gif" /></p></td></tr><tr><td align="left"><p>8/7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.33</mn><mo>±</mo><mn>0.02</mn><mo>±</mo><mn>0.02</mn><mo>±</mo><mn>0.04</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1041.gif" /> (0.05)</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.43</mn><mo>±</mo><mn>0.01</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1042.gif" /></p></td></tr></tbody></table> </ephtml> </p> <p>Graph: Fig. 10 Ratios of tt¯ production cross-sections at different energies: aR13/7tt¯, bR13/8tt¯. The bands show the experimental measurements with the statistical (inner yellow bands), statistical plus experimental and theoretical systematic (middle cyan bands) and total including luminosity (outer green bands) uncertainties. The black triangles with error bars show the predictions and uncertainties from various PDF sets. The last entry shows the prediction using the PDF4LHC recipe, encompassing the predictions from the CT10, MSTW and NNPDF2.3 PDF sets</p> <p>As discussed in Ref. [[<reflink idref="bib27" id="ref166">27</reflink>]], double ratios of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> to <emph>Z</emph> cross-sections at different energies can be used to reduce the luminosity uncertainty, potentially enhancing the sensitivity to PDF differences. The <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> cross-section at a given energy can be normalised to the corresponding <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>Z</mi><mo stretchy="false">→</mo><mi>ℓ</mi><mi>ℓ</mi></mrow></math> </ephtml> fiducial cross-section <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>σ</mi><mrow><mi>Z</mi><mo stretchy="false">→</mo><mi>ℓ</mi><mi>ℓ</mi></mrow><mi mathvariant="normal">fid</mi></msubsup></math> </ephtml> at the same energy by defining the ratio <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi>R</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo stretchy="false">/</mo><mi>Z</mi></mrow></msup></math> </ephtml> as:</p> <p>8 <ephtml> <math display="block" xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtable><mtr><mtd columnalign="right"><mrow><msup><mi>R</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo stretchy="false">/</mo><mi>Z</mi></mrow></msup><mo>=</mo><mfrac><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub><mrow><mn>0.5</mn><mfenced close=")" open="(" separators=""><msubsup><mi>σ</mi><mrow><mi>Z</mi><mo stretchy="false">→</mo><mi>e</mi><mi>e</mi></mrow><mi mathvariant="normal">fid</mi></msubsup><mo>+</mo><msubsup><mi>σ</mi><mrow><mi>Z</mi><mo stretchy="false">→</mo><mi>μ</mi><mi>μ</mi></mrow><mi mathvariant="normal">fid</mi></msubsup></mfenced></mrow></mfrac><mo>,</mo></mrow></mtd></mtr></mtable></mrow></math> </ephtml></p> <p>Graph</p> <p>where the use of the unweighted average of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>Z</mi><mo stretchy="false">→</mo><mi>e</mi><mi>e</mi></mrow></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>Z</mi><mo stretchy="false">→</mo><mi>μ</mi><mi>μ</mi></mrow></math> </ephtml> cross-sections maximises the potential cancellation of electron- and muon-related systematic uncertainties when the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> cross-section is measured using events with one electron and one muon. Provided that the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> and <emph>Z</emph> cross-sections are measured using the same data sample, the integrated luminosity uncertainty cancels almost completely in the ratio <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi>R</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo stretchy="false">/</mo><mi>Z</mi></mrow></msup></math> </ephtml> . Double ratios <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>R</mi><mrow><mi>i</mi><mo stretchy="false">/</mo><mi>j</mi></mrow><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo stretchy="false">/</mo><mi>Z</mi></mrow></msubsup></math> </ephtml> of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi>R</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo stretchy="false">/</mo><mi>Z</mi></mrow></msup></math> </ephtml> at two different energies <emph>i</emph> and <emph>j</emph> can then be defined:</p> <p> <ephtml> <math display="block" xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtable><mtr><mtd columnalign="right"><mrow><msubsup><mi>R</mi><mrow><mi>i</mi><mo stretchy="false">/</mo><mi>j</mi></mrow><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo stretchy="false">/</mo><mi>Z</mi></mrow></msubsup><mo>=</mo><mfrac><mrow><msup><mi>R</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo stretchy="false">/</mo><mi>Z</mi></mrow></msup><mrow><mo stretchy="false">(</mo><mi>i</mi><mo stretchy="false">)</mo></mrow></mrow><mrow><msup><mi>R</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo stretchy="false">/</mo><mi>Z</mi></mrow></msup><mrow><mo stretchy="false">(</mo><mi>j</mi><mo stretchy="false">)</mo></mrow></mrow></mfrac><mo>,</mo></mrow></mtd></mtr></mtable></mrow></math> </ephtml> </p> <p>Graph</p> <p>which benefit from cancellations of uncertainties between beam energies and production processes. In Ref. [[<reflink idref="bib27" id="ref167">27</reflink>]], the previous measurement of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> at <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> from Ref. [[<reflink idref="bib9" id="ref168">9</reflink>]] was used together with the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>7</mn></mrow></math> </ephtml> and 8 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> measurements from Refs. [[<reflink idref="bib7" id="ref169">7</reflink>]] and corresponding measurements of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>σ</mi><mrow><mi>Z</mi><mo stretchy="false">→</mo><mi>ℓ</mi><mi>ℓ</mi></mrow><mi mathvariant="normal">fid</mi></msubsup></math> </ephtml> at each energy to derive double ratios <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>R</mi><mrow><mn>13</mn><mo stretchy="false">/</mo><mn>7</mn></mrow><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo stretchy="false">/</mo><mi>Z</mi></mrow></msubsup></math> </ephtml> , <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>R</mi><mrow><mn>13</mn><mo stretchy="false">/</mo><mn>8</mn></mrow><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo stretchy="false">/</mo><mi>Z</mi></mrow></msubsup></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>R</mi><mrow><mn>8</mn><mo stretchy="false">/</mo><mn>7</mn></mrow><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo stretchy="false">/</mo><mi>Z</mi></mrow></msubsup></math> </ephtml> , which were compared with the predictions from various PDF sets. The <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>Z</mi><mo stretchy="false">→</mo><mi>ℓ</mi><mi>ℓ</mi></mrow></math> </ephtml> cross-sections were measured in a fiducial volume corresponding to the lepton acceptance ( <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub><mo>></mo><mn>25</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mo stretchy="false">|</mo><mi>η</mi><mo stretchy="false">|</mo><mo><</mo><mn>2.5</mn></mrow></math> </ephtml> ) with the dilepton invariant mass in the range <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mn>66</mn><mo><</mo><msub><mi>m</mi><mrow><mi>ℓ</mi><mi>ℓ</mi></mrow></msub><mo><</mo><mn>116</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math> </ephtml> .</p> <p>The precision of the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo stretchy="false">/</mo><mi>Z</mi></mrow></math> </ephtml> ratio and double ratios involving <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> data were limited by the 4.4% uncertainty in the corresponding <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> measurement. These ratios have therefore been updated using the more precise <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> measurement shown in Table 5. The result from 2015 data alone (with an uncertainty of 2.8%) was used in order to maintain the cancellation of luminosity uncertainties in Eq. (<reflink idref="bib8" id="ref170">8</reflink>), as the corresponding <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>σ</mi><mrow><mi>Z</mi><mo stretchy="false">→</mo><mi>ℓ</mi><mi>ℓ</mi></mrow><mi mathvariant="normal">fid</mi></msubsup></math> </ephtml> measurements only used the 2015 data sample. Since the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> result was derived using reoptimised lepton identification and updated calibrations, the lepton uncertainties were conservatively treated as uncorrelated between the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> and <emph>Z</emph> measurements. The largest uncertainties in the double ratio are associated with <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> modelling, and these were treated in the same way as for the updated <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> cross-section ratios discussed above, including the 0.46% increase of the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> value corresponding to the use of a Powheg + Pythia6 CT10 nominal <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> simulation sample. All other uncertainties were treated according to the correlation model described in Ref. [[<reflink idref="bib27" id="ref171">27</reflink>]], with the LHC beam energy uncertainties updated according to Ref. [[<reflink idref="bib88" id="ref172">88</reflink>]]. The input cross-sections are summarised in Table 8.</p> <p>The resulting single and double ratios are shown in Table 10, together with the predictions using the CT14 PDF set, calculated as described in Ref. [[<reflink idref="bib27" id="ref173">27</reflink>]]. The total uncertainties are 1.7% for <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>R</mi><mn>13</mn><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo stretchy="false">/</mo><mi>Z</mi></mrow></msubsup></math> </ephtml> , 3.0% for <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>R</mi><mrow><mn>13</mn><mo stretchy="false">/</mo><mn>7</mn></mrow><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo stretchy="false">/</mo><mi>Z</mi></mrow></msubsup></math> </ephtml> and 2.5% for <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>R</mi><mrow><mn>13</mn><mo stretchy="false">/</mo><mn>8</mn></mrow><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo stretchy="false">/</mo><mi>Z</mi></mrow></msubsup></math> </ephtml> , which are significant improvements on the corresponding uncertainties of 3.5%, 3.8% and 3.6% in Ref. [[<reflink idref="bib27" id="ref174">27</reflink>]]. The largest uncertainties come from the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> measurements, in particular the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> modelling uncertainties, which are mainly treated as uncorrelated between beam energies. Excluding PDF uncertainties, where the correlations between beam energies are fully accounted for, <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> modelling uncertainties contribute 1.7% and 1.4% to the uncertainties on the ratios <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>R</mi><mrow><mn>13</mn><mo stretchy="false">/</mo><mn>7</mn></mrow><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo stretchy="false">/</mo><mi>Z</mi></mrow></msubsup></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>R</mi><mrow><mn>13</mn><mo stretchy="false">/</mo><mn>8</mn></mrow><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo stretchy="false">/</mo><mi>Z</mi></mrow></msubsup></math> </ephtml> . In principle, these uncertainties could be reduced by using a fully coherent set of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> simulation samples and uncertainty model at all beam energies, but that has not been attempted here.</p> <p>The results are compared with the predictions of the ABM12LHC, CT14, NNPDF3.0, MMHT, ATLAS-epWZ12 and HERAPDF2.0 PDF sets (the same sets as in Ref. [[<reflink idref="bib27" id="ref175">27</reflink>]]) in Fig. 11. The measurement of the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo stretchy="false">/</mo><mi>Z</mi></mrow></math> </ephtml> cross-section ratio at <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> is compatible with all the predictions within two standard deviations. Although the experimental uncertainty is only 1.7%, the predictions have common uncertainties of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mrow /><mrow><mo>-</mo><mn>4.6</mn></mrow><mrow><mo>+</mo><mn>4.0</mn></mrow></msubsup></math> </ephtml> % from QCD scale and top quark mass variations, limiting the sensitivity to PDF variations. The pattern for the double ratios is similar to that seen for the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> -only ratios in Fig. 10; the normalisation to <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>Z</mi><mo stretchy="false">→</mo><mi>ℓ</mi><mi>ℓ</mi></mrow></math> </ephtml> cross-sections serves mainly to reduce the luminosity-related uncertainties. The double ratio <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>R</mi><mrow><mn>13</mn><mo stretchy="false">/</mo><mn>7</mn></mrow><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo stretchy="false">/</mo><mi>Z</mi></mrow></msubsup></math> </ephtml> lies below all the predictions, and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>R</mi><mrow><mn>13</mn><mo stretchy="false">/</mo><mn>8</mn></mrow><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo stretchy="false">/</mo><mi>Z</mi></mrow></msubsup></math> </ephtml> lies above all the predictions except that of ABM12LHC. However, the measurements are consistent with all the predictions within two standard deviations, with the exception of ABM12LHC for <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>R</mi><mrow><mn>13</mn><mo stretchy="false">/</mo><mn>7</mn></mrow><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo stretchy="false">/</mo><mi>Z</mi></mrow></msubsup></math> </ephtml> . Similar trends were seen in Ref. [[<reflink idref="bib27" id="ref176">27</reflink>]], although with less separation between PDFs due to the larger uncertainties in the double ratios.</p> <p>Measurements of the ratio of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo stretchy="false">/</mo><mi>Z</mi></mrow></math> </ephtml> cross-sections at <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> , and double ratios of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo stretchy="false">/</mo><mi>Z</mi></mrow></math> </ephtml> cross-sections at <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>7</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> or <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>8</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> , compared with predictions using the CT14 PDF set. The three uncertainties in the measurements are due to data statistics, experimental and theoretical systematic effects (including the small uncertainty due to the LHC beam energy uncertainties) and knowledge of the integrated luminosities of the data samples. The total uncertainty is given in parentheses after each result</p> <p> <ephtml> <table frame="hsides" rules="groups"><thead><tr><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><msqrt xmlns=""><mi>s</mi></msqrt></math><inline-graphic href="10052_2020_7907_Article_IEq1118.gif" /> value (<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1119.gif" />)</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo stretchy="false">/</mo><mi>Z</mi></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1120.gif" /> cross-section ratio</p></th><th align="left"><p>CT14 prediction</p></th></tr></thead><tbody><tr><td align="left"><p>13</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.062</mn><mo>±</mo><mn>0.009</mn><mo>±</mo><mn>0.016</mn><mo>±</mo><mn>0.002</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1121.gif" /> (0.018)</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1</mn><mo>.</mo><msubsup><mn>132</mn><mrow><mo>-</mo><mn>0.075</mn></mrow><mrow><mo>+</mo><mn>0.078</mn></mrow></msubsup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1122.gif" /></p></td></tr></tbody></table> </ephtml> </p> <p>Measurements of the ratio of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo stretchy="false">/</mo><mi>Z</mi></mrow></math> </ephtml> cross-sections at <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> , and double ratios of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo stretchy="false">/</mo><mi>Z</mi></mrow></math> </ephtml> cross-sections at <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>7</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> or <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>8</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> , compared with predictions using the CT14 PDF set. The three uncertainties in the measurements are due to data statistics, experimental and theoretical systematic effects (including the small uncertainty due to the LHC beam energy uncertainties) and knowledge of the integrated luminosities of the data samples. The total uncertainty is given in parentheses after each result</p> <p> <ephtml> <table frame="hsides" rules="groups"><thead><tr><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><msqrt xmlns=""><mi>s</mi></msqrt></math><inline-graphic href="10052_2020_7907_Article_IEq1123.gif" /> values (<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1124.gif" />)</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo stretchy="false">/</mo><mi>Z</mi></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1125.gif" /> cross-section double ratio</p></th><th align="left" /></tr></thead><tbody><tr><td align="left"><p>13/7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.617</mn><mo>±</mo><mn>0.049</mn><mo>±</mo><mn>0.060</mn><mo>±</mo><mn>0.007</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1126.gif" /> (0.078)</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2</mn><mo>.</mo><msubsup><mn>691</mn><mrow><mo>-</mo><mn>0.058</mn></mrow><mrow><mo>+</mo><mn>0.045</mn></mrow></msubsup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1127.gif" /></p></td></tr><tr><td align="left"><p>13/8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.212</mn><mo>±</mo><mn>0.024</mn><mo>±</mo><mn>0.049</mn><mo>±</mo><mn>0.006</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1128.gif" /> (0.055)</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2</mn><mo>.</mo><msubsup><mn>124</mn><mrow><mo>-</mo><mn>0.035</mn></mrow><mrow><mo>+</mo><mn>0.026</mn></mrow></msubsup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1129.gif" /></p></td></tr></tbody></table> </ephtml> </p> <p>Graph: Fig. 11 a Ratio of tt¯ to Z production cross-sections at s=13Te, and double ratios of tt¯ to Z production cross-sections at different energies: bR13/7tt¯/Z, cR13/8tt¯/Z. The bands show the experimental measurements with the statistical (inner yellow bands), statistical plus experimental and theoretical systematic (middle cyan bands) and total including luminosity (barely visible outer green bands) uncertainties. The black triangles with error bars show the predictions and uncertainties from various PDF sets. The s=13Te results use only the 3.2 fb-1 data sample recorded in 2015</p> <hd id="AN0144642803-20">Differential cross-section results</hd> <p>The single-lepton and dilepton absolute fiducial differential cross-section results were obtained by solving Eq. (<reflink idref="bib2" id="ref177">2</reflink>) for each bin <emph>i</emph> of each distribution, using the combined 2015–2016 data sample. The normalised differential cross-sections were obtained from the absolute results using Eq. (<reflink idref="bib3" id="ref178">3</reflink>) and (<reflink idref="bib4" id="ref179">4</reflink>). As in the inclusive cross-section analysis, the results were found to be stable when varying the jet <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> , <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mo stretchy="false">|</mo><mi>η</mi><mo stretchy="false">|</mo></mrow></math> </ephtml> and <emph>b</emph>-tagging requirements. The single-lepton <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>ℓ</mi></msubsup></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>η</mi><mi>ℓ</mi></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> distributions were also measured for electrons and muons separately, instead of combining them into lepton distributions with two entries per event, and found to be compatible. The distributions of bin-by-bin differences in the electron and muon differential cross-sections have <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi>χ</mi><mn>2</mn></msup></math> </ephtml> per degree of freedom of 7/10 for <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>ℓ</mi></msubsup></math> </ephtml> and 13/8 for <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>η</mi><mi>ℓ</mi></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> , in both cases taking statistical and uncorrelated systematic uncertainties into account.</p> <hd id="AN0144642803-21">Results for measured distributions</hd> <p>The measured absolute and normalised fiducial differential cross-sections are shown in Table 15 ( <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>ℓ</mi></msubsup></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>η</mi><mi>ℓ</mi></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> ), Table 16 ( <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mrow><mi>e</mi><mi>μ</mi></mrow></msubsup></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></math> </ephtml> ), Table 17 ( <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>y</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi mathvariant="normal">Δ</mi><msup><mi>ϕ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math> </ephtml> ) and Table 18 ( <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>e</mi></msubsup><mo>+</mo><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>μ</mi></msubsup></mrow></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msup><mi>E</mi><mi>e</mi></msup><mo>+</mo><msup><mi>E</mi><mi>μ</mi></msup></mrow></math> </ephtml> ) in the Appendix. The double-differential cross-sections are shown in Tables 19, 20 ( <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>η</mi><mi>ℓ</mi></msup><mrow><mo stretchy="false">|</mo><mo>×</mo></mrow><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math> </ephtml> ), Tables 21, 22 ( <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>y</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mrow><mo stretchy="false">|</mo><mo>×</mo></mrow><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math> </ephtml> ) and Tables 23, 24 ( <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo><mi mathvariant="normal">Δ</mi></mrow><msup><mi>ϕ</mi><mi>ℓ</mi></msup><mrow><mo stretchy="false">|</mo><mo>×</mo></mrow><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math> </ephtml> ). These tables show the measured cross-section values and uncertainties, together with a breakdown of the total uncertainties into components corresponding to data statistics ('Stat'), <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> modelling (' <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> mod.'), lepton identification and measurement ('Lept.'), jet and <emph>b</emph>-tagging uncertainties ('Jet/<emph>b</emph>'), background uncertainties ('Bkg.') and luminosity/beam energy uncertainties (' <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>L</mi><mo stretchy="false">/</mo><msub><mi>E</mi><mi mathvariant="normal">b</mi></msub></mrow></math> </ephtml> '), matching the categories described in Sects. 5.1–5.5. The rightmost columns show the cross-sections corrected using Eq. (<reflink idref="bib5" id="ref180">5</reflink>) to remove the contributions where at least one lepton results from a leptonic decay of a <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mi>τ</mi></math> </ephtml> -lepton. As also visible in Fig. 6, the total uncertainties in the normalised differential cross-sections range from 0.6% to around 10%, and are typically around half those for the corresponding distributions measured at <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>8</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> [[<reflink idref="bib29" id="ref181">29</reflink>]]. The largest uncertainties are generally statistical, but background uncertainties (in particular from <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover><mo stretchy="false">/</mo><mi>W</mi><mi>t</mi></mrow></math> </ephtml> interference) become dominant at the high ends of the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>ℓ</mi></msubsup></math> </ephtml> , <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mrow><mi>e</mi><mi>μ</mi></mrow></msubsup></math> </ephtml> , <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></math> </ephtml> , <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>e</mi></msubsup><mo>+</mo><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>μ</mi></msubsup></mrow></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msup><mi>E</mi><mi>e</mi></msup><mo>+</mo><msup><mi>E</mi><mi>μ</mi></msup></mrow></math> </ephtml> distributions, and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> modelling uncertainties from the comparison of aMC@NLO + Pythia8 and Powheg + Pythia8 are dominant for most of the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi mathvariant="normal">Δ</mi><msup><mi>ϕ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math> </ephtml> distribution. Uncertainties related to leptons and jets generally play only a minor role; in particular those due to jet energy measurement and <emph>b</emph>-tagging are suppressed due to the determination of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>ϵ</mi><mi>b</mi></msub></math> </ephtml> from data in Eq. (<reflink idref="bib2" id="ref182">2</reflink>). The systematic uncertainties in the normalised differential cross-sections benefit from significant cancellations between bins, and the uncertainties in the absolute cross-sections are substantially larger. The latter also suffer from the uncertainties in the integrated luminosity and beam energy, which contribute 2.3–2.8%, depending on the background level in each bin.</p> <p>The measured normalised differential cross-sections are shown graphically in Figs. 12, 13, 14, 15. The different <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></math> </ephtml> bins for the double-differential cross-sections are shown sequentially on the <emph>x</emph> axes, separated by vertical dotted lines. The measured cross-sections are compared with the particle-level predictions from the baseline Powheg + Pythia8 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> sample, Powheg + Pythia8 samples with more or less parton-shower radiation, and aMC@NLO + Pythia8. The trends seen are similar to those visible in the reconstructed distributions shown in Figs. 1 and 2, and are discussed in the context of comparisons with a larger set of samples in the following.</p> <p>Graph: Fig. 12 Normalised differential cross-sections as a function of apTℓ, b|ηℓ|, cpTeμ and dmeμ. The measured values are shown by the black points with error bars corresponding to the data statistical uncertainties and cyan bands corresponding to the total uncertainties in each bin, and include the contributions via W→τ→e/μ decays. The data points are placed at the centre of each bin. The results are compared with the predictions from the baseline Powheg + Pythia8tt¯ sample, Powheg + Pythia8 samples with more or less parton-shower radiation (RadUp and RadDn), and an aMC@NLO + Pythia8 sample. The lower plots show the ratios of predictions to data, with the error bars indicating the data statistical uncertainties and the cyan bands indicating the total uncertainties in the measurements</p> <p>Graph: Fig. 13 Normalised differential cross-sections as a function of a|yeμ|, bΔϕeμ, cpTe+pTμ and dEe+Eμ. The measured values are shown by the black points with error bars corresponding to the data statistical uncertainties and cyan bands corresponding to the total uncertainties in each bin, and include the contributions via W→τ→e/μ decays. The data points are placed at the centre of each bin. The results are compared with the predictions from the baseline Powheg + Pythia8tt¯ sample, Powheg + Pythia8 samples with more or less parton-shower radiation (RadUp and RadDn), and an aMC@NLO + Pythia8 sample. The lower plots show the ratios of predictions to data, with the error bars indicating the data statistical uncertainties and the cyan bands indicating the total uncertainties in the measurements</p> <p>Graph: Fig. 14 Normalised double-differential cross-sections as functions of |ηℓ| and meμ (top), and |yeμ| and meμ (bottom). The measured values are shown by the black points with error bars corresponding to the data statistical uncertainties and cyan bands corresponding to the total uncertainties in each bin, and include the contributions via W→τ→e/μ decays. The data points are placed at the centre of each bin. The results are compared with the predictions from the baseline Powheg + Pythia8tt¯ sample, Powheg + Pythia8 samples with more or less parton-shower radiation (RadUp and RadDn), and an aMC@NLO + Pythia8 sample. The lower plots show the ratios of predictions to data, with the error bars indicating the data statistical uncertainties and the cyan bands indicating the total uncertainties in the measurements</p> <p>Graph: Fig. 15 Normalised double-differential cross-sections as a function of Δϕeμ and meμ. The measured values are shown by the black points with error bars corresponding to the data statistical uncertainties and cyan bands corresponding to the total uncertainties in each bin, and include the contributions via W→τ→e/μ decays. The data points are placed at the centre of each bin. The results are compared with the predictions from the baseline Powheg + Pythia8tt¯ sample, Powheg + Pythia8 samples with more or less parton-shower radiation (RadUp and RadDn), and an aMC@NLO + Pythia8 sample. The lower plots show the ratios of predictions to data, with the error bars indicating the data statistical uncertainties and the cyan bands indicating the total uncertainties in the measurements</p> <hd id="AN0144642803-22">Comparison with event generator predictions</hd> <p>The measured normalised differential cross-sections are compared to a set of particle-level predictions from different Monte Carlo <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> event generator configurations in Figs. 16, 17, 18, 19, 20, 21, 22. These figures show the ratios of each prediction to the data as functions of the differential variables, with the comparison organised into the four groups of samples summarised in Table 11. These include samples based on Powheg or aMC@NLO for the NLO matrix-element generator, interfaced to Pythia8, Pythia6 or Herwig7, and using various PDF sets. As well as NNPDF3.0 [[<reflink idref="bib44" id="ref183">44</reflink>]] used for the baseline samples, the global NLO PDF sets CT10 [[<reflink idref="bib18" id="ref184">18</reflink>]], CT14 [[<reflink idref="bib74" id="ref185">74</reflink>]], MMHT14 [[<reflink idref="bib77" id="ref186">77</reflink>]] and PDF4LHC_NLO_30 [[<reflink idref="bib76" id="ref187">76</reflink>]] are shown, together with the HERAPDF 2.0 PDF set, based mainly on deep inelastic scattering data [[<reflink idref="bib105" id="ref188">105</reflink>]]. Furthermore, the Powheg + Pythia8 samples with more (denoted 'RadUp') or less ('RadDn') parton-shower radiation described in Sect. 2 are included, together with samples which differ from the baseline Powheg + Pythia8 configuration only by changes of the factorisation and renormalisation scales <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>μ</mi><mi mathvariant="normal">F</mi></msub></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>μ</mi><mi mathvariant="normal">R</mi></msub></math> </ephtml> up and down by factors of two.</p> <p>Summary of particle-level simulation samples used in the comparison with the corrected data distributions in Sect. 7.2, giving the matrix-element event generator, PDF set, parton shower and associated tune parameter set, and other relevant settings. The top quark mass was set to <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>m</mi><mi>t</mi></msub><mo>=</mo><mn>172.5</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math> </ephtml> in all samples. The four groups shown correspond to the four panels for each measured distribution shown in Figs. 16, 17, 18, 19, 20, 21, 22. The baseline Powheg + Pythia8 configuration appears in both groups 1 and 3</p> <p> <ephtml> <table frame="hsides" rules="groups"><thead><tr><th align="left" /><th align="left"><p>Matrix element</p></th><th align="left"><p>PDF</p></th><th align="left"><p>Parton shower/tune</p></th><th align="left"><p>Comments</p></th></tr></thead><tbody><tr><td align="left" rowspan="4"><p>1</p></td><td align="left"><p><sc>Powheg</sc></p></td><td align="left"><p>NNPDF3.0</p></td><td align="left"><p><sc>Pythia8</sc> A14</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msub><mi>h</mi><mi mathvariant="normal">damp</mi></msub><mo>=</mo><mfrac><mn>3</mn><mn>2</mn></mfrac><msub><mi>m</mi><mi>t</mi></msub></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1200.gif" /></p></td></tr><tr><td align="left"><p><sc>Powheg</sc></p></td><td align="left"><p>CT10</p></td><td align="left"><p><sc>Pythia6</sc> P2012</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msub><mi>h</mi><mi mathvariant="normal">damp</mi></msub><mo>=</mo><msub><mi>m</mi><mi>t</mi></msub></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1201.gif" /></p></td></tr><tr><td align="left"><p><sc>Powheg</sc></p></td><td align="left"><p>NNPDF3.0</p></td><td align="left"><p><sc>Herwig7</sc> H7UE</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msub><mi>h</mi><mi mathvariant="normal">damp</mi></msub><mo>=</mo><mfrac><mn>3</mn><mn>2</mn></mfrac><msub><mi>m</mi><mi>t</mi></msub></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1202.gif" /></p></td></tr><tr><td align="left"><p><sc>Powheg</sc></p></td><td align="left"><p>NNPDF3.0</p></td><td align="left"><p><sc>Pythia8</sc> A14</p></td><td align="left"><p>top quark <math xmlns="http://www.w3.org/1998/Math/MathML"><msub xmlns=""><mi>p</mi><mi mathvariant="normal">T</mi></msub></math><inline-graphic href="10052_2020_7907_Article_IEq1203.gif" /> reweighted to Ref. [<xref ref-type="bibr" rid="bibr92">92</xref>]</p></td></tr><tr><td align="left" rowspan="4"><p>2</p></td><td align="left"><p><sc>Powheg</sc></p></td><td align="left"><p>NNPDF3.0</p></td><td align="left"><p><sc>Pythia8</sc> A14v3cDo</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msub><mi>h</mi><mi mathvariant="normal">damp</mi></msub><mo>=</mo><mfrac><mn>3</mn><mn>2</mn></mfrac><msub><mi>m</mi><mi>t</mi></msub></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1204.gif" />, <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2</mn><msub><mi>μ</mi><mrow><mi mathvariant="normal">F</mi><mo>,</mo><mi mathvariant="normal">R</mi></mrow></msub></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1205.gif" /> (RadDn)</p></td></tr><tr><td align="left"><p><sc>Powheg</sc></p></td><td align="left"><p>NNPDF3.0</p></td><td align="left"><p><sc>Pythia8</sc> A14v3cUp</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msub><mi>h</mi><mi mathvariant="normal">damp</mi></msub><mo>=</mo><mn>3</mn><msub><mi>m</mi><mi>t</mi></msub></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1206.gif" />, <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mfrac><mn>1</mn><mn>2</mn></mfrac><msub><mi>μ</mi><mrow><mi mathvariant="normal">F</mi><mo>,</mo><mi mathvariant="normal">R</mi></mrow></msub></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1207.gif" /> (RadUp)</p></td></tr><tr><td align="left"><p><sc>Powheg</sc></p></td><td align="left"><p>NNPDF3.0</p></td><td align="left"><p><sc>Pythia8</sc> A14</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msub><mi>h</mi><mi mathvariant="normal">damp</mi></msub><mo>=</mo><mfrac><mn>3</mn><mn>2</mn></mfrac><msub><mi>m</mi><mi>t</mi></msub></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1208.gif" />, <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2</mn><msub><mi>μ</mi><mrow><mi mathvariant="normal">F</mi><mo>,</mo><mi mathvariant="normal">R</mi></mrow></msub></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1209.gif" /></p></td></tr><tr><td align="left"><p><sc>Powheg</sc></p></td><td align="left"><p>NNPDF3.0</p></td><td align="left"><p><sc>Pythia8</sc> A14</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msub><mi>h</mi><mi mathvariant="normal">damp</mi></msub><mo>=</mo><mfrac><mn>3</mn><mn>2</mn></mfrac><msub><mi>m</mi><mi>t</mi></msub></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1210.gif" />, <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mfrac><mn>1</mn><mn>2</mn></mfrac><msub><mi>μ</mi><mrow><mi mathvariant="normal">F</mi><mo>,</mo><mi mathvariant="normal">R</mi></mrow></msub></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1211.gif" /></p></td></tr><tr><td align="left" rowspan="4"><p>3</p></td><td align="left"><p><sc>Powheg</sc></p></td><td align="left"><p>NNPDF3.0</p></td><td align="left"><p><sc>Pythia8</sc> A14</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msub><mi>h</mi><mi mathvariant="normal">damp</mi></msub><mo>=</mo><mfrac><mn>3</mn><mn>2</mn></mfrac><msub><mi>m</mi><mi>t</mi></msub></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1212.gif" /></p></td></tr><tr><td align="left"><p><sc>Powheg</sc></p></td><td align="left"><p>PDF4LHC15</p></td><td align="left"><p><sc>Pythia8</sc> A14</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msub><mi>h</mi><mi mathvariant="normal">damp</mi></msub><mo>=</mo><mfrac><mn>3</mn><mn>2</mn></mfrac><msub><mi>m</mi><mi>t</mi></msub></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1213.gif" /></p></td></tr><tr><td align="left"><p><sc>Powheg</sc></p></td><td align="left"><p>CT14</p></td><td align="left"><p><sc>Pythia8</sc> A14</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msub><mi>h</mi><mi mathvariant="normal">damp</mi></msub><mo>=</mo><mfrac><mn>3</mn><mn>2</mn></mfrac><msub><mi>m</mi><mi>t</mi></msub></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1214.gif" /></p></td></tr><tr><td align="left"><p><sc>Powheg</sc></p></td><td align="left"><p>MMHT</p></td><td align="left"><p><sc>Pythia8</sc> A14</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msub><mi>h</mi><mi mathvariant="normal">damp</mi></msub><mo>=</mo><mfrac><mn>3</mn><mn>2</mn></mfrac><msub><mi>m</mi><mi>t</mi></msub></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1215.gif" /></p></td></tr><tr><td align="left" rowspan="3"><p>4</p></td><td align="left"><p><sc>aMC@NLO</sc></p></td><td align="left"><p>NNPDF3.0</p></td><td align="left"><p><sc>Pythia8</sc> A14</p></td><td align="left" /></tr><tr><td align="left"><p><sc>aMC@NLO</sc></p></td><td align="left"><p>CT10</p></td><td align="left"><p><sc>Pythia8</sc> A14</p></td><td align="left" /></tr><tr><td align="left"><p><sc>aMC@MLO</sc></p></td><td align="left"><p>HERAPDF2.0</p></td><td align="left"><p><sc>Pythia8</sc> A14</p></td><td align="left" /></tr></tbody></table> </ephtml> </p> <p>The baseline Powheg + Pythia8 configuration is known to predict too hard a top quark <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> distribution compared to data at <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> [[<reflink idref="bib92" id="ref189">92</reflink>]] and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>8</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> [[<reflink idref="bib106" id="ref190">106</reflink>]], and compared to NNLO QCD calculations [[<reflink idref="bib107" id="ref191">107</reflink>]]. To explore the effect of this mismodelling on the lepton differential distributions, the Powheg + Pythia8 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> sample was reweighted according to the top quark <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> in each event, using a linear function whose parameters were chosen so as to reproduce the measured top quark <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> distribution shown in Figure 19 of Ref. [[<reflink idref="bib92" id="ref192">92</reflink>]]; this sample is included in the first sample group and labelled 'Powheg + PY8 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> rew' in Figs. 16, 17, 18, 19, 20, 21, 22.</p> <p>Graph: Fig. 16 Ratios of predictions of normalised differential cross-sections to data as a function of apTℓ and b|ηℓ|. The data statistical uncertainties are shown by the black error bars around a ratio of unity, and the total uncertainties are shown by the cyan bands. Several different tt¯ predictions are shown in each panel, grouped from top to bottom as shown in Table 11, and the error bars indicate the uncertainties due to the limited size of the simulated samples</p> <p>Graph: Fig. 17 Ratios of predictions of normalised differential cross-sections to data as a function of apTeμ and bmeμ. The data statistical uncertainties are shown by the black error bars around a ratio of unity, and the total uncertainties are shown by the cyan bands. Several different tt¯ predictions are shown in each panel, grouped from top to bottom as shown in Table 11, and the error bars indicate the uncertainties due to the limited size of the simulated samples</p> <p>Graph: Fig. 18 Ratios of predictions of normalised differential cross-sections to data as a function of a|yeμ| and bΔϕeμ. The data statistical uncertainties are shown by the black error bars around a ratio of unity, and the total uncertainties are shown by the cyan bands. Several different tt¯ predictions are shown in each panel, grouped from top to bottom as shown in Table 11, and the error bars indicate the uncertainties due to the limited size of the simulated samples</p> <p>Graph: Fig. 19 Ratios of predictions of normalised differential cross-sections to data as a function of apTe+pTμ and bEe+Eμ. The data statistical uncertainties are shown by the black error bars around a ratio of unity, and the total uncertainties are shown by the cyan bands. Several different tt¯ predictions are shown in each panel, grouped from top to bottom as shown in Table 11, and the error bars indicate the uncertainties due to the limited size of the simulated samples</p> <p>Graph: Fig. 20 Ratios of predictions of the normalised double-differential cross-sections to data as a function of |ηℓ| and meμ. The data statistical uncertainties are shown by the black error bars around a ratio of unity, and the total uncertainties are shown by the cyan bands. The vertical dotted lines indicate the four bins of meμ. Several different tt¯ predictions are shown in each panel, grouped from top to bottom as shown in Table 11, and the error bars indicate the uncertainties due to the limited size of the simulated samples</p> <p>Graph: Fig. 21 Ratios of predictions of the normalised double-differential cross-sections to data as a function of |yeμ| and meμ. The data statistical uncertainties are shown by the black error bars around a ratio of unity, and the total uncertainties are shown by the cyan bands. The vertical dotted lines indicate the four bins of meμ. Several different tt¯ predictions are shown in each panel, grouped from top to bottom as shown in Table 11, and the error bars indicate the uncertainties due to the limited size of the simulated samples</p> <p>Graph: Fig. 22 Ratios of predictions of the normalised double-differential cross-sections to data as a function of Δϕeμ and meμ. The data statistical uncertainties are shown by the black error bars around a ratio of unity, and the total uncertainties are shown by the cyan bands. The vertical dotted lines indicate the four bins of meμ. Several different tt¯ predictions are shown in each panel, grouped from top to bottom as shown in Table 11, and the error bars indicate the uncertainties due to the limited size of the simulated samples</p> <p>The compatibility of each prediction with each measured normalised distribution was tested using a <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi>χ</mi><mn>2</mn></msup></math> </ephtml> calculated as</p> <p>9 <ephtml> <math display="block" xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtable><mtr><mtd columnalign="right"><mrow><msup><mi>χ</mi><mn>2</mn></msup><mo>=</mo><msubsup><mrow><mi mathvariant="bold">Δ</mi></mrow><mrow><mo stretchy="false">(</mo><mi>n</mi><mo>-</mo><mn>1</mn><mo stretchy="false">)</mo></mrow><mi>T</mi></msubsup><msubsup><mrow><mi mathvariant="bold">S</mi></mrow><mrow><mo stretchy="false">(</mo><mi>n</mi><mo>-</mo><mn>1</mn><mo stretchy="false">)</mo></mrow><mrow><mo>-</mo><mn>1</mn></mrow></msubsup><msub><mrow><mi mathvariant="bold">Δ</mi></mrow><mrow><mo stretchy="false">(</mo><mi>n</mi><mo>-</mo><mn>1</mn><mo stretchy="false">)</mo></mrow></msub><mspace width="0.166667em" /><mo>,</mo></mrow></mtd></mtr></mtable></mrow></math> </ephtml></p> <p>Graph</p> <p>where <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mrow><mi mathvariant="bold">Δ</mi></mrow><mrow><mo stretchy="false">(</mo><mi>n</mi><mo>-</mo><mn>1</mn><mo stretchy="false">)</mo></mrow></msub></math> </ephtml> is the vector of differences between the measured and predicted normalised differential cross-section in each of the <emph>n</emph> bins, excluding the last one, and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mrow><mi mathvariant="bold">S</mi></mrow><mrow><mo stretchy="false">(</mo><mi>n</mi><mo>-</mo><mn>1</mn><mo stretchy="false">)</mo></mrow><mrow><mo>-</mo><mn>1</mn></mrow></msubsup></math> </ephtml> is the inverse of the corresponding covariance matrix, including both the experimental uncertainties in the measurement and the statistical uncertainties in the predictions. Correlations between the measurements in different bins were incorporated via off-diagonal terms in <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mi mathvariant="bold">S</mi></math> </ephtml> , and the last bin of each distribution was excluded to account for the degree of freedom lost to the normalisation condition. The resulting <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi>χ</mi><mn>2</mn></msup></math> </ephtml> values and corresponding probability <emph>p</emph>-values (for <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>n</mi><mo>-</mo><mn>1</mn></mrow></math> </ephtml> degrees of freedom) are shown for each single-differential distribution and prediction in Table 12, and for the double-differential distributions and predictions in Table 13.</p> <p> <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi>χ</mi><mn>2</mn></msup></math> </ephtml> values (top) and associated probabilities (bottom) for comparison of normalised measured single-differential fiducial cross-sections with various <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> simulation samples. Probabilities smaller than <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mn>10</mn><mrow><mo>-</mo><mn>10</mn></mrow></msup></math> </ephtml> are shown as zero</p> <p> <ephtml> <table frame="hsides" rules="groups"><thead><tr><th align="left"><p>Generator</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup xmlns=""><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>ℓ</mi></msubsup></math><inline-graphic href="10052_2020_7907_Article_IEq1258.gif" /></p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mrow><mo stretchy="false">|</mo></mrow><msup><mi>η</mi><mi>ℓ</mi></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1259.gif" /></p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup xmlns=""><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mrow><mi>e</mi><mi>μ</mi></mrow></msubsup></math><inline-graphic href="10052_2020_7907_Article_IEq1260.gif" /></p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><msup xmlns=""><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></math><inline-graphic href="10052_2020_7907_Article_IEq1261.gif" /></p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mrow><mo stretchy="false">|</mo></mrow><msup><mi>y</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1262.gif" /></p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi mathvariant="normal">Δ</mi><msup><mi>ϕ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1263.gif" /></p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>e</mi></msubsup><mo>+</mo><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>μ</mi></msubsup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1264.gif" /></p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msup><mi>E</mi><mi>e</mi></msup><mo>+</mo><msup><mi>E</mi><mi>μ</mi></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1265.gif" /></p></th></tr><tr><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><msub xmlns=""><mi>N</mi><mi mathvariant="normal">dof</mi></msub></math><inline-graphic href="10052_2020_7907_Article_IEq1266.gif" /></p></th><th align="left"><p>10</p></th><th align="left"><p>8</p></th><th align="left"><p>8</p></th><th align="left"><p>11</p></th><th align="left"><p>8</p></th><th align="left"><p>9</p></th><th align="left"><p>7</p></th><th align="left"><p>9</p></th></tr></thead><tbody><tr><td align="left"><p><sc>Powheg + PY8</sc></p></td><td align="left"><p>43.7</p></td><td align="left"><p>19.5</p></td><td align="left"><p>8.6</p></td><td align="left"><p>44.3</p></td><td align="left"><p>11.4</p></td><td align="left"><p>14.4</p></td><td align="left"><p>32.5</p></td><td align="left"><p>18.4</p></td></tr><tr><td align="left"><p><sc>Powheg + PY6</sc> CT10</p></td><td align="left"><p>36.1</p></td><td align="left"><p>7.9</p></td><td align="left"><p>9.3</p></td><td align="left"><p>33.0</p></td><td align="left"><p>16.2</p></td><td align="left"><p>16.2</p></td><td align="left"><p>21.9</p></td><td align="left"><p>30.5</p></td></tr><tr><td align="left"><p><sc>Powheg + HW7</sc></p></td><td align="left"><p>34.8</p></td><td align="left"><p>15.9</p></td><td align="left"><p>11.5</p></td><td align="left"><p>62.7</p></td><td align="left"><p>9.4</p></td><td align="left"><p>17.3</p></td><td align="left"><p>23.0</p></td><td align="left"><p>14.7</p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc><math xmlns="http://www.w3.org/1998/Math/MathML"><msub xmlns=""><mi>p</mi><mi mathvariant="normal">T</mi></msub></math><inline-graphic href="10052_2020_7907_Article_IEq1267.gif" /> rew.</p></td><td align="left"><p>20.2</p></td><td align="left"><p>14.7</p></td><td align="left"><p>2.3</p></td><td align="left"><p>38.3</p></td><td align="left"><p>8.4</p></td><td align="left"><p>12.7</p></td><td align="left"><p>9.4</p></td><td align="left"><p>14.0</p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc> RadDn</p></td><td align="left"><p>40.0</p></td><td align="left"><p>24.2</p></td><td align="left"><p>6.1</p></td><td align="left"><p>44.3</p></td><td align="left"><p>9.2</p></td><td align="left"><p>16.3</p></td><td align="left"><p>29.0</p></td><td align="left"><p>20.1</p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc> RadUp</p></td><td align="left"><p>33.0</p></td><td align="left"><p>16.3</p></td><td align="left"><p>21.9</p></td><td align="left"><p>35.3</p></td><td align="left"><p>12.3</p></td><td align="left"><p>6.4</p></td><td align="left"><p>26.7</p></td><td align="left"><p>16.5</p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msub><mi>μ</mi><mrow><mi mathvariant="normal">F</mi><mo>,</mo><mi mathvariant="normal">R</mi></mrow></msub><mo>×</mo><mn>2</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1268.gif" /></p></td><td align="left"><p>46.5</p></td><td align="left"><p>21.6</p></td><td align="left"><p>6.2</p></td><td align="left"><p>42.6</p></td><td align="left"><p>8.5</p></td><td align="left"><p>16.5</p></td><td align="left"><p>28.9</p></td><td align="left"><p>17.1</p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msub><mi>μ</mi><mrow><mi mathvariant="normal">F</mi><mo>,</mo><mi mathvariant="normal">R</mi></mrow></msub><mo>×</mo><mn>0.5</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1269.gif" /></p></td><td align="left"><p>39.8</p></td><td align="left"><p>17.3</p></td><td align="left"><p>11.4</p></td><td align="left"><p>38.0</p></td><td align="left"><p>10.7</p></td><td align="left"><p>10.9</p></td><td align="left"><p>27.6</p></td><td align="left"><p>14.2</p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc> PDF4LHC15</p></td><td align="left"><p>43.4</p></td><td align="left"><p>14.6</p></td><td align="left"><p>7.4</p></td><td align="left"><p>39.0</p></td><td align="left"><p>6.2</p></td><td align="left"><p>13.5</p></td><td align="left"><p>28.0</p></td><td align="left"><p>15.9</p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc> CT14</p></td><td align="left"><p>44.1</p></td><td align="left"><p>9.3</p></td><td align="left"><p>7.6</p></td><td align="left"><p>37.0</p></td><td align="left"><p>8.2</p></td><td align="left"><p>13.5</p></td><td align="left"><p>28.5</p></td><td align="left"><p>18.2</p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc> MMHT</p></td><td align="left"><p>41.2</p></td><td align="left"><p>17.7</p></td><td align="left"><p>6.9</p></td><td align="left"><p>39.0</p></td><td align="left"><p>6.3</p></td><td align="left"><p>13.2</p></td><td align="left"><p>26.3</p></td><td align="left"><p>14.3</p></td></tr><tr><td align="left"><p><sc>aMC@NLO + PY8</sc></p></td><td align="left"><p>26.2</p></td><td align="left"><p>25.7</p></td><td align="left"><p>11.4</p></td><td align="left"><p>19.7</p></td><td align="left"><p>16.7</p></td><td align="left"><p>13.2</p></td><td align="left"><p>12.5</p></td><td align="left"><p>14.0</p></td></tr><tr><td align="left"><p><sc>aMC@NLO + PY8</sc> CT10</p></td><td align="left"><p>24.9</p></td><td align="left"><p>11.7</p></td><td align="left"><p>10.6</p></td><td align="left"><p>16.9</p></td><td align="left"><p>10.0</p></td><td align="left"><p>13.4</p></td><td align="left"><p>12.0</p></td><td align="left"><p>19.0</p></td></tr><tr><td align="left"><p><sc>aMC@NLO + PY8</sc> HERA2</p></td><td align="left"><p>17.1</p></td><td align="left"><p>96.6</p></td><td align="left"><p>6.9</p></td><td align="left"><p>26.0</p></td><td align="left"><p>68.5</p></td><td align="left"><p>12.5</p></td><td align="left"><p>6.1</p></td><td align="left"><p>38.4</p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>6</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1270.gif" /></p></td><td align="left"><p>0.012</p></td><td align="left"><p>0.37</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>6</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>6</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1271.gif" /></p></td><td align="left"><p>0.18</p></td><td align="left"><p>0.11</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>5</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1272.gif" /></p></td><td align="left"><p>0.030</p></td></tr><tr><td align="left"><p><sc>Powheg + PY6</sc> CT10</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>8</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>5</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1273.gif" /></p></td><td align="left"><p>0.45</p></td><td align="left"><p>0.32</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>5</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>4</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1274.gif" /></p></td><td align="left"><p>0.039</p></td><td align="left"><p>0.062</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>3</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1275.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>4</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1276.gif" /></p></td></tr><tr><td align="left"><p><sc>Powheg + HW7</sc></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>4</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1277.gif" /></p></td><td align="left"><p>0.043</p></td><td align="left"><p>0.18</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>9</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1278.gif" /></p></td><td align="left"><p>0.31</p></td><td align="left"><p>0.045</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>3</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1279.gif" /></p></td><td align="left"><p>0.098</p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc><math xmlns="http://www.w3.org/1998/Math/MathML"><msub xmlns=""><mi>p</mi><mi mathvariant="normal">T</mi></msub></math><inline-graphic href="10052_2020_7907_Article_IEq1280.gif" /> rew.</p></td><td align="left"><p>0.028</p></td><td align="left"><p>0.065</p></td><td align="left"><p>0.97</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>7</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>5</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1281.gif" /></p></td><td align="left"><p>0.39</p></td><td align="left"><p>0.18</p></td><td align="left"><p>0.23</p></td><td align="left"><p>0.12</p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc> RadDn</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>5</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1282.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>3</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1283.gif" /></p></td><td align="left"><p>0.64</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>6</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>6</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1284.gif" /></p></td><td align="left"><p>0.32</p></td><td align="left"><p>0.060</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>4</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1285.gif" /></p></td><td align="left"><p>0.017</p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc> RadUp</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>4</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1286.gif" /></p></td><td align="left"><p>0.038</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>5</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>3</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1287.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>4</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1288.gif" /></p></td><td align="left"><p>0.14</p></td><td align="left"><p>0.70</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>4</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1289.gif" /></p></td><td align="left"><p>0.057</p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msub><mi>μ</mi><mrow><mi mathvariant="normal">F</mi><mo>,</mo><mi mathvariant="normal">R</mi></mrow></msub><mo>×</mo><mn>2</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1290.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>6</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1291.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>6</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>3</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1292.gif" /></p></td><td align="left"><p>0.62</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>5</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1293.gif" /></p></td><td align="left"><p>0.39</p></td><td align="left"><p>0.056</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>4</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1294.gif" /></p></td><td align="left"><p>0.048</p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msub><mi>μ</mi><mrow><mi mathvariant="normal">F</mi><mo>,</mo><mi mathvariant="normal">R</mi></mrow></msub><mo>×</mo><mn>0.5</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1295.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>5</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1296.gif" /></p></td><td align="left"><p>0.027</p></td><td align="left"><p>0.18</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>8</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>5</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1297.gif" /></p></td><td align="left"><p>0.22</p></td><td align="left"><p>0.28</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>4</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1298.gif" /></p></td><td align="left"><p>0.12</p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc> PDF4LHC15</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>6</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1299.gif" /></p></td><td align="left"><p>0.067</p></td><td align="left"><p>0.49</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>5</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>5</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1300.gif" /></p></td><td align="left"><p>0.62</p></td><td align="left"><p>0.14</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>4</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1301.gif" /></p></td><td align="left"><p>0.068</p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc> CT14</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>6</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1302.gif" /></p></td><td align="left"><p>0.32</p></td><td align="left"><p>0.47</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>4</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1303.gif" /></p></td><td align="left"><p>0.42</p></td><td align="left"><p>0.14</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>4</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1304.gif" /></p></td><td align="left"><p>0.033</p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc> MMHT</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>5</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1305.gif" /></p></td><td align="left"><p>0.024</p></td><td align="left"><p>0.55</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>5</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>5</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1306.gif" /></p></td><td align="left"><p>0.62</p></td><td align="left"><p>0.15</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>5</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>4</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1307.gif" /></p></td><td align="left"><p>0.11</p></td></tr><tr><td align="left"><p><sc>aMC@NLO + PY8</sc></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>3</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1308.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>3</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1309.gif" /></p></td><td align="left"><p>0.18</p></td><td align="left"><p>0.049</p></td><td align="left"><p>0.034</p></td><td align="left"><p>0.15</p></td><td align="left"><p>0.086</p></td><td align="left"><p>0.12</p></td></tr><tr><td align="left"><p><sc>aMC@NLO + PY8</sc> CT10</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>5</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>3</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1310.gif" /></p></td><td align="left"><p>0.16</p></td><td align="left"><p>0.23</p></td><td align="left"><p>0.11</p></td><td align="left"><p>0.27</p></td><td align="left"><p>0.15</p></td><td align="left"><p>0.10</p></td><td align="left"><p>0.025</p></td></tr><tr><td align="left"><p><sc>aMC@NLO + PY8</sc> HERA2</p></td><td align="left"><p>0.073</p></td><td align="left"><p>0</p></td><td align="left"><p>0.54</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>6</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>3</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1311.gif" /></p></td><td align="left"><p>0</p></td><td align="left"><p>0.19</p></td><td align="left"><p>0.53</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>5</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1312.gif" /></p></td></tr></tbody></table> </ephtml> </p> <p> <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi>χ</mi><mn>2</mn></msup></math> </ephtml> values (top) and associated probabilities (bottom) for comparison of normalised measured double-differential fiducial cross-sections with various <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> simulation samples. Probabilities smaller than <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mn>10</mn><mrow><mo>-</mo><mn>10</mn></mrow></msup></math> </ephtml> are shown as zero</p> <p> <ephtml> <table frame="hsides" rules="groups"><thead><tr><th align="left"><p>Generator</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mrow><mo stretchy="false">|</mo></mrow><msup><mi>η</mi><mi>ℓ</mi></msup><mrow><mo stretchy="false">|</mo><mo>×</mo></mrow><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1316.gif" /></p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mrow><mo stretchy="false">|</mo></mrow><msup><mi>y</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mrow><mo stretchy="false">|</mo><mo>×</mo></mrow><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1317.gif" /></p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mrow><mo stretchy="false">|</mo><mi mathvariant="normal">Δ</mi></mrow><msup><mi>ϕ</mi><mi>ℓ</mi></msup><mrow><mo stretchy="false">|</mo><mo>×</mo></mrow><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1318.gif" /></p></th></tr><tr><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><msub xmlns=""><mi>N</mi><mi mathvariant="normal">dof</mi></msub></math><inline-graphic href="10052_2020_7907_Article_IEq1319.gif" /></p></th><th align="left"><p>35</p></th><th align="left"><p>19</p></th><th align="left"><p>39</p></th></tr></thead><tbody><tr><td align="left"><p><sc>Powheg + PY8</sc></p></td><td align="left"><p>53.1</p></td><td align="left"><p>72.3</p></td><td align="left"><p>65.4</p></td></tr><tr><td align="left"><p><sc>Powheg + PY6</sc> CT10</p></td><td align="left"><p>45.9</p></td><td align="left"><p>92.9</p></td><td align="left"><p>79.5</p></td></tr><tr><td align="left"><p><sc>Powheg + HW7</sc></p></td><td align="left"><p>49.3</p></td><td align="left"><p>67.4</p></td><td align="left"><p>63.7</p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc><math xmlns="http://www.w3.org/1998/Math/MathML"><msub xmlns=""><mi>p</mi><mi mathvariant="normal">T</mi></msub></math><inline-graphic href="10052_2020_7907_Article_IEq1320.gif" /> rew.</p></td><td align="left"><p>47.1</p></td><td align="left"><p>56.1</p></td><td align="left"><p>51.4</p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc> RadDn</p></td><td align="left"><p>57.1</p></td><td align="left"><p>74.2</p></td><td align="left"><p>69.9</p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc> RadUp</p></td><td align="left"><p>50.6</p></td><td align="left"><p>62.5</p></td><td align="left"><p>51.7</p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msub><mi>μ</mi><mrow><mi mathvariant="normal">F</mi><mo>,</mo><mi mathvariant="normal">R</mi></mrow></msub><mo>×</mo><mn>2</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1321.gif" /></p></td><td align="left"><p>60.7</p></td><td align="left"><p>68.4</p></td><td align="left"><p>71.1</p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msub><mi>μ</mi><mrow><mi mathvariant="normal">F</mi><mo>,</mo><mi mathvariant="normal">R</mi></mrow></msub><mo>×</mo><mn>0.5</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1322.gif" /></p></td><td align="left"><p>50.3</p></td><td align="left"><p>60.0</p></td><td align="left"><p>52.0</p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc> PDF4LHC15</p></td><td align="left"><p>51.5</p></td><td align="left"><p>61.5</p></td><td align="left"><p>59.7</p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc> CT14</p></td><td align="left"><p>50.6</p></td><td align="left"><p>67.3</p></td><td align="left"><p>60.0</p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc> MMHT</p></td><td align="left"><p>53.7</p></td><td align="left"><p>57.9</p></td><td align="left"><p>58.7</p></td></tr><tr><td align="left"><p><sc>aMC@NLO + PY8</sc></p></td><td align="left"><p>55.0</p></td><td align="left"><p>45.9</p></td><td align="left"><p>58.2</p></td></tr><tr><td align="left"><p><sc>aMC@NLO + PY8</sc> CT10</p></td><td align="left"><p>43.7</p></td><td align="left"><p>50.6</p></td><td align="left"><p>59.5</p></td></tr><tr><td align="left"><p><sc>aMC@NLO + PY8</sc> HERA2</p></td><td align="left"><p>130.3</p></td><td align="left"><p>97.6</p></td><td align="left"><p>58.0</p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc></p></td><td align="left"><p>0.026</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>8</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1323.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>5</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>3</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1324.gif" /></p></td></tr><tr><td align="left"><p><sc>Powheg + PY6</sc> CT10</p></td><td align="left"><p>0.10</p></td><td align="left"><p>0</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>4</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1325.gif" /></p></td></tr><tr><td align="left"><p><sc>Powheg + HW7</sc></p></td><td align="left"><p>0.055</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>7</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1326.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>8</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>3</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1327.gif" /></p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc><math xmlns="http://www.w3.org/1998/Math/MathML"><msub xmlns=""><mi>p</mi><mi mathvariant="normal">T</mi></msub></math><inline-graphic href="10052_2020_7907_Article_IEq1328.gif" /> rew.</p></td><td align="left"><p>0.084</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>5</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1329.gif" /></p></td><td align="left"><p>0.088</p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc> RadDn</p></td><td align="left"><p>0.011</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>8</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1330.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>3</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1331.gif" /></p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc> RadUp</p></td><td align="left"><p>0.042</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>6</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1332.gif" /></p></td><td align="left"><p>0.083</p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msub><mi>μ</mi><mrow><mi mathvariant="normal">F</mi><mo>,</mo><mi mathvariant="normal">R</mi></mrow></msub><mo>×</mo><mn>2</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1333.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>5</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>3</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1334.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>7</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1335.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>3</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1336.gif" /></p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msub><mi>μ</mi><mrow><mi mathvariant="normal">F</mi><mo>,</mo><mi mathvariant="normal">R</mi></mrow></msub><mo>×</mo><mn>0.5</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1337.gif" /></p></td><td align="left"><p>0.045</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>6</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1338.gif" /></p></td><td align="left"><p>0.079</p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc> PDF4LHC15</p></td><td align="left"><p>0.036</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>6</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1339.gif" /></p></td><td align="left"><p>0.018</p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc> CT14</p></td><td align="left"><p>0.042</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>7</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1340.gif" /></p></td><td align="left"><p>0.017</p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc> MMHT</p></td><td align="left"><p>0.023</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>8</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>6</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1341.gif" /></p></td><td align="left"><p>0.022</p></td></tr><tr><td align="left"><p><sc>aMC@NLO + PY8</sc></p></td><td align="left"><p>0.017</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>5</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>4</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1342.gif" /></p></td><td align="left"><p>0.024</p></td></tr><tr><td align="left"><p><sc>aMC@NLO + PY8</sc> CT10</p></td><td align="left"><p>0.15</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>4</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1343.gif" /></p></td><td align="left"><p>0.019</p></td></tr><tr><td align="left"><p><sc>aMC@NLO + PY8</sc> HERA2</p></td><td align="left"><p>0</p></td><td align="left"><p>0</p></td><td align="left"><p>0.026</p></td></tr></tbody></table> </ephtml> </p> <p>A number of observations can be made for the modelling of the individual lepton and dilepton distributions. The single-lepton <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> and dilepton <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>e</mi></msubsup><mo>+</mo><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>μ</mi></msubsup></mrow></math> </ephtml> distributions (Figs. 16a, 19a) are softer in the data than in all the Powheg-based predictions, irrespective of the choice of parton shower, scale/tune settings or PDF. The aMC@NLO + Pythia8 samples agree better with data, especially when using the HERAPDF2.0 PDF set. Reweighting the top quark <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> in the Powheg + Pythia8 sample also gives significantly better agreement. Similar features were seen in the comparisons of the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>ℓ</mi></msubsup></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>e</mi></msubsup><mo>+</mo><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>μ</mi></msubsup></mrow></math> </ephtml> distributions at <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>8</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> [[<reflink idref="bib29" id="ref193">29</reflink>]], and in the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>ℓ</mi></msubsup></math> </ephtml> distribution measured by CMS at <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> in a different fiducial region including requirements on jets [[<reflink idref="bib108" id="ref194">108</reflink>]].</p> <p>The single-lepton <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>η</mi><mi>ℓ</mi></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> distribution (Fig. 16b) is more forward than the predictions from either Powheg + Pythia8 or aMC@NLO + Pythia8 with the NNPDF3.0 set, and agreement is improved by using CT10 or CT14. The MMHT and PDF4LHC15 PDF sets lie somewhere in between, but HERAPDF2.0 predicts much too central a distribution. The <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>y</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> distribution (Fig. 18a) shows a slightly different picture; again HERAPDF2.0 is in very poor agreement with the data, but all the other PDFs do reasonably well. These observations differ from those at <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>8</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> [[<reflink idref="bib29" id="ref195">29</reflink>]], where the HERAPDF 1.5 and 2.0 PDF sets were found to describe the data better than CT10, which was used as the default.</p> <p>All the generators model the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mrow><mi>e</mi><mi>μ</mi></mrow></msubsup></math> </ephtml> distribution well (Fig. 17a), with the exception of the Powheg + Pythia8 RadUp configuration, and to a lesser extent, Powheg + Pythia8 with reduced QCD scales. This distribution shows little sensitivity to PDFs. The <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></math> </ephtml> distribution (Fig. 17b) is poorly modelled by all Powheg-based samples. The aMC@NLO + Pythia8 samples do better (except when HERAPDF2.0 is used), but still fail to describe the data at very low <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></math> </ephtml> .</p> <p>The data have a less steep <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi mathvariant="normal">Δ</mi><msup><mi>ϕ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math> </ephtml> distribution than all the predictions (Fig. 18b), although the Powheg + Pythia8 RadUp and reduced QCD scale samples come close, as does the sample with reweighted top quark <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> . The tensions between data and predictions are smaller than in the dedicated ATLAS <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> spin correlation analysis [[<reflink idref="bib109" id="ref196">109</reflink>]], but the latter analysis has a more restrictive fiducial region definition, with higher lepton <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> thresholds and a requirement of at least two jets.</p> <p>Finally, the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msup><mi>E</mi><mi>e</mi></msup><mo>+</mo><msup><mi>E</mi><mi>μ</mi></msup></mrow></math> </ephtml> distribution (Fig. 19b) is reasonably described by the baseline Powheg + Pythia8 prediction except at high <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msup><mi>E</mi><mi>e</mi></msup><mo>+</mo><msup><mi>E</mi><mi>μ</mi></msup></mrow></math> </ephtml> , where agreement is improved by top quark <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> reweighting. The distribution shows some sensitivity to PDFs, with NNPDF3.0 agreeing with data better than CT10, and HERAPDF2.0 again agreeing very poorly with data.</p> <p>The comparisons of normalised double-differential cross-section measurements and predictions in Figs. 20, 21, 22 reflect those seen in the single-differential results, although generally with reduced significance due to the larger per-bin statistical uncertainties. The <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi>χ</mi><mn>2</mn></msup></math> </ephtml> and probabilities shown in Table 13 are all poor, driven by poor agreement of the measured <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></math> </ephtml> distribution and predictions already visible in Fig. 17b. The largest differences between the models are seen at low <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></math> </ephtml> for <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>η</mi><mi>ℓ</mi></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> , whereas the differences become more pronounced at high <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></math> </ephtml> for <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>y</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> . Similar trends in <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi mathvariant="normal">Δ</mi><msup><mi>ϕ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math> </ephtml> are visible in all <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></math> </ephtml> bins in Fig. 22, despite the shape of the overall <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi mathvariant="normal">Δ</mi><msup><mi>ϕ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math> </ephtml> distribution changing significantly across the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></math> </ephtml> bins, as shown in Fig. 15. This distribution is again best described by the Powheg + Pythia8 predictions with increased radiation (RadUp), reduced QCD scales, or reweighted top quark <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> .</p> <p>The <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi>χ</mi><mn>2</mn></msup></math> </ephtml> computation of Eq. (<reflink idref="bib9" id="ref197">9</reflink>) was extended to consider several normalised distributions simultaneously. The statistical correlations between distributions were evaluated using pseudo-experiments, and systematic uncertainties were assumed to be correlated between distributions. Five sets of combined distributions were considered: <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>ℓ</mi></msubsup></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mrow><mi>e</mi><mi>μ</mi></mrow></msubsup></math> </ephtml> ; <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mrow><mi>e</mi><mi>μ</mi></mrow></msubsup></math> </ephtml> , <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>e</mi></msubsup><mo>+</mo><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>μ</mi></msubsup></mrow></math> </ephtml> ; <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>η</mi><mi>ℓ</mi></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>y</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> ; <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>η</mi><mi>ℓ</mi></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> , <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>y</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msup><mi>E</mi><mi>e</mi></msup><mo>+</mo><msup><mi>E</mi><mi>μ</mi></msup></mrow></math> </ephtml> ; and the combination of all eight single-differential distributions.</p> <p> <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi>χ</mi><mn>2</mn></msup></math> </ephtml> values (top) and associated probabilities (bottom) for comparison of combinations of measured normalised differential fiducial cross-sections with various <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> simulation samples. The last column gives the results for the combination of all eight measured single-differential distributions. Probabilities smaller than <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mn>10</mn><mrow><mo>-</mo><mn>10</mn></mrow></msup></math> </ephtml> are shown as zero</p> <p> <ephtml> <table frame="hsides" rules="groups"><thead><tr><th align="left"><p>Generator</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup xmlns=""><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>ℓ</mi></msubsup></math><inline-graphic href="10052_2020_7907_Article_IEq1393.gif" />, <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>e</mi></msubsup><mo>+</mo><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>μ</mi></msubsup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1394.gif" /></p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup xmlns=""><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mrow><mi>e</mi><mi>μ</mi></mrow></msubsup></math><inline-graphic href="10052_2020_7907_Article_IEq1395.gif" />, <math xmlns="http://www.w3.org/1998/Math/MathML"><msup xmlns=""><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></math><inline-graphic href="10052_2020_7907_Article_IEq1396.gif" />,</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mrow><mo stretchy="false">|</mo></mrow><msup><mi>η</mi><mi>ℓ</mi></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1397.gif" />, <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mrow><mo stretchy="false">|</mo></mrow><msup><mi>y</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1398.gif" /></p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mrow><mo stretchy="false">|</mo></mrow><msup><mi>η</mi><mi>ℓ</mi></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1399.gif" />, <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mrow><mo stretchy="false">|</mo></mrow><msup><mi>y</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1400.gif" />,</p></th><th align="left"><p>All 8</p></th></tr><tr><th align="left" /><th align="left" /><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>e</mi></msubsup><mo>+</mo><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>μ</mi></msubsup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1401.gif" /></p></th><th align="left" /><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msup><mi>E</mi><mi>e</mi></msup><mo>+</mo><msup><mi>E</mi><mi>μ</mi></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1402.gif" /></p></th><th align="left"><p>dists.</p></th></tr><tr><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><msub xmlns=""><mi>N</mi><mi mathvariant="normal">dof</mi></msub></math><inline-graphic href="10052_2020_7907_Article_IEq1403.gif" /></p></th><th align="left"><p>17</p></th><th align="left"><p>26</p></th><th align="left"><p>16</p></th><th align="left"><p>25</p></th><th align="left"><p>70</p></th></tr></thead><tbody><tr><td align="left"><p><sc>Powheg + PY8</sc></p></td><td align="left"><p>52.2</p></td><td align="left"><p>92.8</p></td><td align="left"><p>31.2</p></td><td align="left"><p>51.5</p></td><td align="left"><p>176.5</p></td></tr><tr><td align="left"><p><sc>Powheg + PY6</sc> CT10</p></td><td align="left"><p>42.9</p></td><td align="left"><p>87.9</p></td><td align="left"><p>31.0</p></td><td align="left"><p>58.0</p></td><td align="left"><p>176.6</p></td></tr><tr><td align="left"><p><sc>Powheg + HW7</sc></p></td><td align="left"><p>42.5</p></td><td align="left"><p>97.4</p></td><td align="left"><p>25.7</p></td><td align="left"><p>41.6</p></td><td align="left"><p>169.8</p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc><math xmlns="http://www.w3.org/1998/Math/MathML"><msub xmlns=""><mi>p</mi><mi mathvariant="normal">T</mi></msub></math><inline-graphic href="10052_2020_7907_Article_IEq1404.gif" /> rew.</p></td><td align="left"><p>27.5</p></td><td align="left"><p>57.4</p></td><td align="left"><p>25.4</p></td><td align="left"><p>36.5</p></td><td align="left"><p>137.6</p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc> RadDn</p></td><td align="left"><p>49.7</p></td><td align="left"><p>110.8</p></td><td align="left"><p>37.8</p></td><td align="left"><p>58.3</p></td><td align="left"><p>193.9</p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc> RadUp</p></td><td align="left"><p>42.9</p></td><td align="left"><p>71.8</p></td><td align="left"><p>25.5</p></td><td align="left"><p>44.2</p></td><td align="left"><p>151.8</p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msub><mi>μ</mi><mrow><mi mathvariant="normal">F</mi><mo>,</mo><mi mathvariant="normal">R</mi></mrow></msub><mo>×</mo><mn>2</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1405.gif" /></p></td><td align="left"><p>54.5</p></td><td align="left"><p>111.1</p></td><td align="left"><p>35.6</p></td><td align="left"><p>54.4</p></td><td align="left"><p>195.0</p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msub><mi>μ</mi><mrow><mi mathvariant="normal">F</mi><mo>,</mo><mi mathvariant="normal">R</mi></mrow></msub><mo>×</mo><mn>0.5</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1406.gif" /></p></td><td align="left"><p>50.5</p></td><td align="left"><p>71.3</p></td><td align="left"><p>26.3</p></td><td align="left"><p>42.8</p></td><td align="left"><p>160.4</p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc> PDF4LHC15</p></td><td align="left"><p>52.2</p></td><td align="left"><p>89.7</p></td><td align="left"><p>26.7</p></td><td align="left"><p>44.1</p></td><td align="left"><p>167.1</p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc> CT14</p></td><td align="left"><p>52.9</p></td><td align="left"><p>91.5</p></td><td align="left"><p>26.6</p></td><td align="left"><p>44.8</p></td><td align="left"><p>170.2</p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc> MMHT</p></td><td align="left"><p>49.9</p></td><td align="left"><p>89.4</p></td><td align="left"><p>28.7</p></td><td align="left"><p>44.8</p></td><td align="left"><p>167.6</p></td></tr><tr><td align="left"><p><sc>aMC@NLO + PY8</sc></p></td><td align="left"><p>33.2</p></td><td align="left"><p>46.3</p></td><td align="left"><p>37.1</p></td><td align="left"><p>49.6</p></td><td align="left"><p>131.9</p></td></tr><tr><td align="left"><p><sc>aMC@NLO + PY8</sc> CT10</p></td><td align="left"><p>31.6</p></td><td align="left"><p>46.7</p></td><td align="left"><p>26.2</p></td><td align="left"><p>43.0</p></td><td align="left"><p>122.9</p></td></tr><tr><td align="left"><p><sc>aMC@NLO + PY8</sc> HERA2</p></td><td align="left"><p>23.1</p></td><td align="left"><p>51.5</p></td><td align="left"><p>119.0</p></td><td align="left"><p>132.8</p></td><td align="left"><p>229.8</p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>5</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1407.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>9</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1408.gif" /></p></td><td align="left"><p>0.013</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>3</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1409.gif" /></p></td><td align="left"><p>0</p></td></tr><tr><td align="left"><p><sc>Powheg + PY6</sc> CT10</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>5</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>4</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1410.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>8</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1411.gif" /></p></td><td align="left"><p>0.014</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>4</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1412.gif" /></p></td><td align="left"><p>0</p></td></tr><tr><td align="left"><p><sc>Powheg + HW7</sc></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>6</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>4</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1413.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>10</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1414.gif" /></p></td><td align="left"><p>0.058</p></td><td align="left"><p>0.020</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>10</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1415.gif" /></p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc><math xmlns="http://www.w3.org/1998/Math/MathML"><msub xmlns=""><mi>p</mi><mi mathvariant="normal">T</mi></msub></math><inline-graphic href="10052_2020_7907_Article_IEq1416.gif" /> rew.</p></td><td align="left"><p>0.052</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>4</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1417.gif" /></p></td><td align="left"><p>0.062</p></td><td align="left"><p>0.064</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>6</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1418.gif" /></p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc> RadDn</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>5</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>5</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1419.gif" /></p></td><td align="left"><p>0</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>3</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1420.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>4</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1421.gif" /></p></td><td align="left"><p>0</p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc> RadUp</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>5</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>4</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1422.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>6</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1423.gif" /></p></td><td align="left"><p>0.062</p></td><td align="left"><p>0.010</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>6</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>8</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1424.gif" /></p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msub><mi>μ</mi><mrow><mi mathvariant="normal">F</mi><mo>,</mo><mi mathvariant="normal">R</mi></mrow></msub><mo>×</mo><mn>2</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1425.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>8</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>6</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1426.gif" /></p></td><td align="left"><p>0</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>3</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1427.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>6</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>4</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1428.gif" /></p></td><td align="left"><p>0</p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msub><mi>μ</mi><mrow><mi mathvariant="normal">F</mi><mo>,</mo><mi mathvariant="normal">R</mi></mrow></msub><mo>×</mo><mn>0.5</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1429.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>5</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1430.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>6</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1431.gif" /></p></td><td align="left"><p>0.049</p></td><td align="left"><p>0.015</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>5</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>9</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1432.gif" /></p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc> PDF4LHC15</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>5</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1433.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>6</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>9</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1434.gif" /></p></td><td align="left"><p>0.045</p></td><td align="left"><p>0.011</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>7</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>10</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1435.gif" /></p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc> CT14</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>5</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1436.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>9</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1437.gif" /></p></td><td align="left"><p>0.046</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>9</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>3</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1438.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>10</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1439.gif" /></p></td></tr><tr><td align="left"><p><sc>Powheg + PY8</sc> MMHT</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>5</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1440.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>7</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>9</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1441.gif" /></p></td><td align="left"><p>0.026</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>9</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>3</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1442.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>6</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>10</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1443.gif" /></p></td></tr><tr><td align="left"><p><sc>aMC@NLO + PY8</sc></p></td><td align="left"><p>0.011</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>9</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>3</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1444.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>3</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1445.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>3</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1446.gif" /></p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>5</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1447.gif" /></p></td></tr><tr><td align="left"><p><sc>aMC@NLO + PY8</sc> CT10</p></td><td align="left"><p>0.017</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>8</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>3</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1448.gif" /></p></td><td align="left"><p>0.051</p></td><td align="left"><p>0.014</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>4</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1449.gif" /></p></td></tr><tr><td align="left"><p><sc>aMC@NLO + PY8</sc> HERA2</p></td><td align="left"><p>0.14</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2</mn><mo>·</mo><msup><mn>10</mn><mrow><mo>-</mo><mn>3</mn></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1450.gif" /></p></td><td align="left"><p>0</p></td><td align="left"><p>0</p></td><td align="left"><p>0</p></td></tr></tbody></table> </ephtml> </p> <p>The resulting <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi>χ</mi><mn>2</mn></msup></math> </ephtml> and <emph>p</emph>-values are shown for each combination and prediction in Table 14. The best descriptions of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>e</mi></msubsup><mo>+</mo><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>μ</mi></msubsup></mrow></math> </ephtml> are achieved by Powheg + Pythia8 with top quark <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> reweighting, or by aMC@NLO + Pythia8, particularly with the HERAPDF2.0 PDF set. Either NLO generator combined with several PDF sets can describe the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>η</mi><mi>ℓ</mi></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>y</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> distributions, although only the sample with top quark <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> reweighting provides a reasonable description once <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msup><mi>E</mi><mi>e</mi></msup><mo>+</mo><msup><mi>E</mi><mi>μ</mi></msup></mrow></math> </ephtml> is also included. No samples describe the combinations including <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></math> </ephtml> , as this variable is not modelled by any of the generator configurations.</p> <hd id="AN0144642803-23">Conclusions</hd> <p>The inclusive <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> production cross-section <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> has been measured in <emph>pp</emph> collisions at <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></mrow></math> </ephtml><ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> using 36.1 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mspace width="0.333333em" /><mtext>fb</mtext><msup><mspace width="0.333333em" /><mrow><mo>-</mo><mn>1</mn></mrow></msup></mrow></math> </ephtml> of data recorded by the ATLAS experiment at the LHC in 2015–2016. Using events with an opposite-sign <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>e</mi><mi>μ</mi></mrow></math> </ephtml> pair and one or two <emph>b</emph>-tagged jets, the result is:</p> <p> <ephtml> <math display="block" xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtable><mtr><mtd columnalign="right"><mrow><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub><mo>=</mo><mn>826.4</mn><mo>±</mo><mn>3.6</mn><mspace width="0.166667em" /><mrow><mo stretchy="false">(</mo><mi mathvariant="normal">stat</mi><mo stretchy="false">)</mo></mrow><mspace width="4pt" /><mo>±</mo><mn>11.5</mn><mspace width="0.166667em" /><mrow><mo stretchy="false">(</mo><mi mathvariant="normal">syst</mi><mo stretchy="false">)</mo></mrow><mspace width="4pt" /><mo>±</mo><mn>15.7</mn><mspace width="0.166667em" /><mrow><mo stretchy="false">(</mo><mi mathvariant="normal">lumi</mi><mo stretchy="false">)</mo></mrow><mspace width="4pt" /><mo>±</mo><mn>1.9</mn><mspace width="0.166667em" /><mrow><mo stretchy="false">(</mo><mi mathvariant="normal">beam</mi><mo stretchy="false">)</mo></mrow><mspace width="0.166667em" /><mi mathvariant="normal">pb</mi><mo>,</mo></mrow></mtd></mtr></mtable></mrow></math> </ephtml> </p> <p>Graph</p> <p>where the four uncertainties are due to data statistics, experimental and theoretical systematic effects, and the knowledge of the integrated luminosity and of the LHC beam energy. The result is consistent with NNLO+NNLL QCD predictions. Fiducial cross-sections corresponding to the experimental acceptance for the leptons, with and without a correction for the contribution of leptons from leptonic <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mi>τ</mi></math> </ephtml> decays, have also been measured. The dependence of predictions for <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> on the top quark pole mass <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>m</mi><mi>t</mi><mi mathvariant="normal">pole</mi></msubsup></math> </ephtml> has been exploited to determine a mass value of</p> <p> <ephtml> <math display="block" xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtable><mtr><mtd columnalign="right"><mrow><msubsup><mi>m</mi><mi>t</mi><mi mathvariant="normal">pole</mi></msubsup><mo>=</mo><mn>173</mn><mo>.</mo><msubsup><mn>1</mn><mrow><mo>-</mo><mn>2.1</mn></mrow><mrow><mo>+</mo><mn>2.0</mn></mrow></msubsup><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></mtd></mtr></mtable></mrow></math> </ephtml> </p> <p>Graph</p> <p>from the inclusive cross-section, using the predictions derived with the CT14 PDF set. This result is compatible with other top quark mass determinations using a variety of techniques. The inclusive cross-section has also been combined with previous measurements at <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>7</mn></mrow></math> </ephtml> and 8 <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mtext>Te</mtext><mspace width="0.333333em" /></mrow></math> </ephtml> to determine ratios of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> cross-sections, and double ratios of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> </ephtml> to <emph>Z</emph> cross-sections, at different energies, which are found to be compatible with predictions using a range of PDF sets.</p> <p>The same data sample has been used to measure eight single-differential and three double-differential cross-sections as a function of lepton and dilepton kinematic variables, with uncertainties as small as 0.6% for normalised distributions in some parts of the fiducial region. The measured distributions are generally well described by the NLO matrix-element generators Powheg and aMC@NLO when interfaced to Pythia or Herwig for parton shower, hadronisation and underlying-event modelling. However, the Powheg-based predictions give lepton <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub></math> </ephtml> spectra that are significantly harder than those observed in data, and none of the predictions describe the low-mass part of the dilepton invariant mass distribution. These differential cross-section results have sensitivity to PDFs and can be used as the basis for a precise determination of the top quark mass based on lepton kinematics.</p> <hd id="AN0144642803-24">Acknowledgements</hd> <p>We thank CERN for the very successful operation of the LHC, as well as the support staff from our institutions without whom ATLAS could not be operated efficiently.</p> <p>We acknowledge the support of ANPCyT, Argentina; YerPhI, Armenia; ARC, Australia; BMWFW and FWF, Austria; ANAS, Azerbaijan; SSTC, Belarus; CNPq and FAPESP, Brazil; NSERC, NRC and CFI, Canada; CERN; CONICYT, Chile; CAS, MOST and NSFC, China; COLCIENCIAS, Colombia; MSMT CR, MPO CR and VSC CR, Czech Republic; DNRF and DNSRC, Denmark; IN2P3-CNRS and CEA-DRF/IRFU, France; SRNSFG, Georgia; BMBF, HGF and MPG, Germany; GSRT, Greece; RGC and Hong Kong SAR, China; ISF and Benoziyo Center, Israel; INFN, Italy; MEXT and JSPS, Japan; CNRST, Morocco; NWO, Netherlands; RCN, Norway; MNiSW and NCN, Poland; FCT, Portugal; MNE/IFA, Romania; MES of Russia and NRC KI, Russia Federation; JINR; MESTD, Serbia; MSSR, Slovakia; ARRS and MIZŠ, Slovenia; DST/NRF, South Africa; MINECO, Spain; SRC and Wallenberg Foundation, Sweden; SERI, SNSF and Cantons of Bern and Geneva, Switzerland; MOST, Taiwan; TAEK, Turkey; STFC, United Kingdom; DOE and NSF, United States of America. In addition, individual groups and members have received support from BCKDF, CANARIE, Compute Canada and CRC, Canada; ERC, ERDF, Horizon 2020, Marie Skłodowska-Curie Actions and COST, European Union; Investissements d'Avenir Labex, Investissements d'Avenir Idex and ANR, France; DFG and AvH Foundation, Germany; Herakleitos, Thales and Aristeia programmes co-financed by EU-ESF and the Greek NSRF, Greece; BSF-NSF and GIF, Israel; CERCA Programme Generalitat de Catalunya and PROMETEO Programme Generalitat Valenciana, Spain; Göran Gustafssons Stiftelse, Sweden; The Royal Society and Leverhulme Trust, United Kingdom.</p> <p>The crucial computing support from all WLCG partners is acknowledged gratefully, in particular from CERN, the ATLAS Tier-1 facilities at TRIUMF (Canada), NDGF (Denmark, Norway, Sweden), CC-IN2P3 (France), KIT/GridKA (Germany), INFN-CNAF (Italy), NL-T1 (Netherlands), PIC (Spain), ASGC (Taiwan), RAL (UK) and BNL (USA), the Tier-2 facilities worldwide and large non-WLCG resource providers. Major contributors of computing resources are listed in Ref. [[<reflink idref="bib110" id="ref198">110</reflink>]].</p> <hd id="AN0144642803-25">Data Availability Statement</hd> <p>This manuscript has no associated data or the data will not be deposited. [Authors' comment: All ATLAS scientific output is published in journals, and preliminary results are made available in Conference Notes. All are openly available, without restriction on use by external parties beyond copyright law and the standard conditions agreed by CERN. Data associated with journal publications are also made available: tables and data from plots (e.g. cross section values, likelihood profiles, selection efficiencies, cross section limits,...) are stored in appropriate repositories such as HEPDATA (<ulink href="http://hepdata.cedar.ac.uk/">http://hepdata.cedar.ac.uk/</ulink>). ATLAS also strives to make additional material related to the paper available that allows a reinterpretation of the data in the context of new theoretical models. For example, an extended encapsulation of the analysis is often provided for measurements in the framework of RIVET (<ulink href="http://rivet.hepforge.org/">http://rivet.hepforge.org/</ulink>). This information is taken from the ATLAS Data Access Policy, which is a public document that can be downloaded from <ulink href="http://opendata.cern.ch/record/413">http://opendata.cern.ch/record/413</ulink> [<ulink href="http://opendata.cern.ch">http://opendata.cern.ch</ulink>].]</p> <hd id="AN0144642803-26">Appendix</hd> <p>The measured absolute and normalised differential cross-sections as functions of individual lepton and dilepton variables are shown in Tables 15, 16, 17, 18. The absolute and normalised double-differential cross-sections as functions of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>η</mi><mi>ℓ</mi></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></math> </ephtml> are shown in Tables 19 and 20, those as a function of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>y</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></math> </ephtml> in Tables 21 and 22, and those as a function of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi mathvariant="normal">Δ</mi><msup><mi>ϕ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></math> </ephtml> in Tables 23 and 24. More details are given in Sect. 7.</p> <p>Absolute and normalised differential cross-sections as functions of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>ℓ</mi></msubsup></math> </ephtml> (top) and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>η</mi><mi>ℓ</mi></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> (bottom). The columns show the bin ranges, measured cross-section and total uncertainty, relative statistical uncertainty, relative systematic uncertainties in various categories (see text), total relative uncertainty, and differential cross-section corrected to remove contributions via <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>W</mi><mo stretchy="false">→</mo><mi>τ</mi><mo stretchy="false">→</mo><mi>e</mi><mo stretchy="false">/</mo><mi>μ</mi></mrow></math> </ephtml> decays. Relative uncertainties smaller than 0.05% are indicated by '0.0'. The last bin includes overflows where indicated by the '+' sign</p> <p> <ephtml> <table frame="hsides" rules="groups"><thead><tr><th align="left"><p>Absolute</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi mathvariant="normal">d</mi><mi>σ</mi><mo stretchy="false">/</mo><mi mathvariant="normal">d</mi><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>ℓ</mi></msubsup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1483.gif" /></p></th><th align="left"><p>Stat.</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1484.gif" /> mod.</p></th><th align="left"><p>Lept.</p></th><th align="left"><p>Jet/<italic>b</italic></p></th><th align="left"><p>Bkg.</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>L</mi><mo stretchy="false">/</mo><msub><mi>E</mi><mi mathvariant="normal">b</mi></msub></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1485.gif" /></p></th><th align="left"><p>Total</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi mathvariant="normal">d</mi><mi>σ</mi><mo stretchy="false">/</mo><mi mathvariant="normal">d</mi><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>ℓ</mi></msubsup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1486.gif" /> (no <math xmlns="http://www.w3.org/1998/Math/MathML"><mi xmlns="">τ</mi></math><inline-graphic href="10052_2020_7907_Article_IEq1487.gif" />)</p></th></tr><tr><th align="left"><p>Bin (<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1488.gif" />)</p></th><th align="left"><p>(fb/<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1489.gif" />)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(fb/<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1490.gif" />)</p></th></tr></thead><tbody><tr><td align="left"><p>20–25</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>564</mn><mo>±</mo><mn>17</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1491.gif" /></p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.9</p></td><td align="left"><p>1.4</p></td><td align="left"><p>0.2</p></td><td align="left"><p>1.0</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.1</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>436</mn><mo>±</mo><mn>13</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1492.gif" /></p></td></tr><tr><td align="left"><p>25–30</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>562</mn><mo>±</mo><mn>16</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1493.gif" /></p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.9</p></td><td align="left"><p>1.1</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.8</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.9</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>456</mn><mo>±</mo><mn>13</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1494.gif" /></p></td></tr><tr><td align="left"><p>30–40</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>525</mn><mo>±</mo><mn>14</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1495.gif" /></p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.7</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>441</mn><mo>±</mo><mn>12</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1496.gif" /></p></td></tr><tr><td align="left"><p>40–50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>428</mn><mo>±</mo><mn>12</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1497.gif" /></p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.7</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>369</mn><mo>±</mo><mn>10</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1498.gif" /></p></td></tr><tr><td align="left"><p>50–60</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>336.2</mn><mo>±</mo><mn>9.2</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1499.gif" /></p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.7</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>294.8</mn><mo>±</mo><mn>7.8</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1500.gif" /></p></td></tr><tr><td align="left"><p>60–80</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>220.6</mn><mo>±</mo><mn>6.0</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1501.gif" /></p></td><td align="left"><p>0.4</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.7</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>195.9</mn><mo>±</mo><mn>5.2</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1502.gif" /></p></td></tr><tr><td align="left"><p>80–100</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>120.1</mn><mo>±</mo><mn>3.4</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1503.gif" /></p></td><td align="left"><p>0.6</p></td><td align="left"><p>1.1</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.8</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.9</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>107.4</mn><mo>±</mo><mn>3.0</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1504.gif" /></p></td></tr><tr><td align="left"><p>100–120</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>66.6</mn><mo>±</mo><mn>2.0</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1505.gif" /></p></td><td align="left"><p>0.8</p></td><td align="left"><p>1.1</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.2</p></td><td align="left"><p>1.0</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.0</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>59.7</mn><mo>±</mo><mn>1.7</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1506.gif" /></p></td></tr><tr><td align="left"><p>120–150</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>30.6</mn><mo>±</mo><mn>1.0</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1507.gif" /></p></td><td align="left"><p>1.0</p></td><td align="left"><p>1.2</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.3</p></td><td align="left"><p>1.5</p></td><td align="left"><p>2.4</p></td><td align="left"><p>3.3</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>27.4</mn><mo>±</mo><mn>0.9</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1508.gif" /></p></td></tr><tr><td align="left"><p>150–200</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>10.80</mn><mo>±</mo><mn>0.45</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1509.gif" /></p></td><td align="left"><p>1.4</p></td><td align="left"><p>1.2</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.2</p></td><td align="left"><p>2.6</p></td><td align="left"><p>2.5</p></td><td align="left"><p>4.1</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>9.64</mn><mo>±</mo><mn>0.39</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1510.gif" /></p></td></tr><tr><td align="left"><p>200–300+</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.33</mn><mo>±</mo><mn>0.20</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1511.gif" /></p></td><td align="left"><p>2.2</p></td><td align="left"><p>1.6</p></td><td align="left"><p>1.5</p></td><td align="left"><p>0.4</p></td><td align="left"><p>7.8</p></td><td align="left"><p>2.6</p></td><td align="left"><p>8.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.07</mn><mo>±</mo><mn>0.18</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1512.gif" /></p></td></tr></tbody></table> </ephtml> </p> <p>Absolute and normalised differential cross-sections as functions of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>ℓ</mi></msubsup></math> </ephtml> (top) and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>η</mi><mi>ℓ</mi></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> (bottom). The columns show the bin ranges, measured cross-section and total uncertainty, relative statistical uncertainty, relative systematic uncertainties in various categories (see text), total relative uncertainty, and differential cross-section corrected to remove contributions via <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>W</mi><mo stretchy="false">→</mo><mi>τ</mi><mo stretchy="false">→</mo><mi>e</mi><mo stretchy="false">/</mo><mi>μ</mi></mrow></math> </ephtml> decays. Relative uncertainties smaller than 0.05% are indicated by '0.0'. The last bin includes overflows where indicated by the '+' sign</p> <p> <ephtml> <table frame="hsides" rules="groups"><thead><tr><th align="left"><p> Normalised</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mfrac><mn>1</mn><mi>σ</mi></mfrac><mi mathvariant="normal">d</mi><mi>σ</mi><mo stretchy="false">/</mo><mi mathvariant="normal">d</mi><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>ℓ</mi></msubsup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1513.gif" /></p></th><th align="left"><p>Stat.</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1514.gif" /> mod.</p></th><th align="left"><p>Lept.</p></th><th align="left"><p>Jet/<italic>b</italic></p></th><th align="left"><p>Bkg.</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>L</mi><mo stretchy="false">/</mo><msub><mi>E</mi><mi mathvariant="normal">b</mi></msub></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1515.gif" /></p></th><th align="left"><p>Total</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mfrac><mn>1</mn><mi>σ</mi></mfrac><mi mathvariant="normal">d</mi><mi>σ</mi><mo stretchy="false">/</mo><mi mathvariant="normal">d</mi><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>ℓ</mi></msubsup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1516.gif" /> (no <math xmlns="http://www.w3.org/1998/Math/MathML"><mi xmlns="">τ</mi></math><inline-graphic href="10052_2020_7907_Article_IEq1517.gif" />)</p></th></tr><tr><th align="left"><p>Bin (<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1518.gif" />)</p></th><th align="left"><p>(<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msup><mn>10</mn><mrow><mo>-</mo><mn>2</mn></mrow></msup><mo stretchy="false">/</mo></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1519.gif" /><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1520.gif" />)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msup><mn>10</mn><mrow><mo>-</mo><mn>2</mn></mrow></msup><mo stretchy="false">/</mo></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1521.gif" /><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1522.gif" />)</p></th></tr></thead><tbody><tr><td align="left"><p>20–25</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.987</mn><mo>±</mo><mn>0.026</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1523.gif" /></p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.3</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.796</mn><mo>±</mo><mn>0.023</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1524.gif" /></p></td></tr><tr><td align="left"><p>25–30</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.982</mn><mo>±</mo><mn>0.019</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1525.gif" /></p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.0</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.876</mn><mo>±</mo><mn>0.018</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1526.gif" /></p></td></tr><tr><td align="left"><p>30–40</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.852</mn><mo>±</mo><mn>0.012</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1527.gif" /></p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.817</mn><mo>±</mo><mn>0.012</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1528.gif" /></p></td></tr><tr><td align="left"><p>40–50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.5095</mn><mo>±</mo><mn>0.0096</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1529.gif" /></p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.6</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.5212</mn><mo>±</mo><mn>0.0097</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1530.gif" /></p></td></tr><tr><td align="left"><p>50–60</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.1855</mn><mo>±</mo><mn>0.0079</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1531.gif" /></p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.2142</mn><mo>±</mo><mn>0.0080</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1532.gif" /></p></td></tr><tr><td align="left"><p>60–80</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.7779</mn><mo>±</mo><mn>0.0047</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1533.gif" /></p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.6</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.8067</mn><mo>±</mo><mn>0.0047</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1534.gif" /></p></td></tr><tr><td align="left"><p>80–100</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.4234</mn><mo>±</mo><mn>0.0035</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1535.gif" /></p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.4423</mn><mo>±</mo><mn>0.0035</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1536.gif" /></p></td></tr><tr><td align="left"><p>100–120</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.2348</mn><mo>±</mo><mn>0.0028</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1537.gif" /></p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.2</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.2459</mn><mo>±</mo><mn>0.0029</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1538.gif" /></p></td></tr><tr><td align="left"><p>120–150</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.1080</mn><mo>±</mo><mn>0.0019</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1539.gif" /></p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.1</p></td><td align="left"><p>1.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>1.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.1129</mn><mo>±</mo><mn>0.0019</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1540.gif" /></p></td></tr><tr><td align="left"><p>150–200</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.0381</mn><mo>±</mo><mn>0.0012</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1541.gif" /></p></td><td align="left"><p>1.3</p></td><td align="left"><p>0.9</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.2</p></td><td align="left"><p>2.4</p></td><td align="left"><p>0.1</p></td><td align="left"><p>3.0</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.0397</mn><mo>±</mo><mn>0.0012</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1542.gif" /></p></td></tr><tr><td align="left"><p>200–300+</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.0082</mn><mo>±</mo><mn>0.0007</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1543.gif" /></p></td><td align="left"><p>2.2</p></td><td align="left"><p>1.6</p></td><td align="left"><p>1.6</p></td><td align="left"><p>0.4</p></td><td align="left"><p>7.6</p></td><td align="left"><p>0.3</p></td><td align="left"><p>8.2</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.0085</mn><mo>±</mo><mn>0.0007</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1544.gif" /></p></td></tr></tbody></table> </ephtml> </p> <p>Absolute and normalised differential cross-sections as functions of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>ℓ</mi></msubsup></math> </ephtml> (top) and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>η</mi><mi>ℓ</mi></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> (bottom). The columns show the bin ranges, measured cross-section and total uncertainty, relative statistical uncertainty, relative systematic uncertainties in various categories (see text), total relative uncertainty, and differential cross-section corrected to remove contributions via <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>W</mi><mo stretchy="false">→</mo><mi>τ</mi><mo stretchy="false">→</mo><mi>e</mi><mo stretchy="false">/</mo><mi>μ</mi></mrow></math> </ephtml> decays. Relative uncertainties smaller than 0.05% are indicated by '0.0'. The last bin includes overflows where indicated by the '+' sign</p> <p> <ephtml> <table frame="hsides" rules="groups"><thead><tr><th align="left"><p> Absolute</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mrow><mi mathvariant="normal">d</mi><mi>σ</mi><mo stretchy="false">/</mo><mi mathvariant="normal">d</mi><mo stretchy="false">|</mo></mrow><msup><mi>η</mi><mi>ℓ</mi></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1545.gif" /></p></th><th align="left"><p>Stat.</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1546.gif" /> mod.</p></th><th align="left"><p>Lept.</p></th><th align="left"><p>Jet/<italic>b</italic></p></th><th align="left"><p>Bkg.</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>L</mi><mo stretchy="false">/</mo><msub><mi>E</mi><mi mathvariant="normal">b</mi></msub></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1547.gif" /></p></th><th align="left"><p>Total</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mrow><mi mathvariant="normal">d</mi><mi>σ</mi><mo stretchy="false">/</mo><mi mathvariant="normal">d</mi><mo stretchy="false">|</mo></mrow><msup><mi>η</mi><mi>ℓ</mi></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1548.gif" /> (no <math xmlns="http://www.w3.org/1998/Math/MathML"><mi xmlns="">τ</mi></math><inline-graphic href="10052_2020_7907_Article_IEq1549.gif" />)</p></th></tr><tr><th align="left"><p>Bin (unit <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mo stretchy="false">|</mo><mi>η</mi><mo stretchy="false">|</mo></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1550.gif" />)</p></th><th align="left"><p>(fb/unit <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mo stretchy="false">|</mo><mi>η</mi><mo stretchy="false">|</mo></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1551.gif" />)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(fb/unit <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mo stretchy="false">|</mo><mi>η</mi><mo stretchy="false">|</mo></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1552.gif" />)</p></th></tr></thead><tbody><tr><td align="left"><p>0.00–0.25</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>17270</mn><mo>±</mo><mn>460</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1553.gif" /></p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.7</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>14750</mn><mo>±</mo><mn>390</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1554.gif" /></p></td></tr><tr><td align="left"><p>0.25–0.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>16520</mn><mo>±</mo><mn>440</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1555.gif" /></p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.7</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>14110</mn><mo>±</mo><mn>370</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1556.gif" /></p></td></tr><tr><td align="left"><p>0.50–0.75</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>15660</mn><mo>±</mo><mn>420</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1557.gif" /></p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.7</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>13390</mn><mo>±</mo><mn>350</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1558.gif" /></p></td></tr><tr><td align="left"><p>0.75–1.00</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>14320</mn><mo>±</mo><mn>390</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1559.gif" /></p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.7</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>12250</mn><mo>±</mo><mn>330</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1560.gif" /></p></td></tr><tr><td align="left"><p>1.00–1.25</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>12660</mn><mo>±</mo><mn>350</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1561.gif" /></p></td><td align="left"><p>0.5</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.8</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>10850</mn><mo>±</mo><mn>290</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1562.gif" /></p></td></tr><tr><td align="left"><p>1.25–1.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>10940</mn><mo>±</mo><mn>310</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1563.gif" /></p></td><td align="left"><p>0.7</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.8</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>9370</mn><mo>±</mo><mn>260</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1564.gif" /></p></td></tr><tr><td align="left"><p>1.50–1.75</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>9090</mn><mo>±</mo><mn>260</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1565.gif" /></p></td><td align="left"><p>0.7</p></td><td align="left"><p>1.1</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.9</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.9</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>7810</mn><mo>±</mo><mn>220</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1566.gif" /></p></td></tr><tr><td align="left"><p>1.75–2.00</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>7320</mn><mo>±</mo><mn>220</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1567.gif" /></p></td><td align="left"><p>0.8</p></td><td align="left"><p>1.2</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.2</p></td><td align="left"><p>1.0</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.0</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>6310</mn><mo>±</mo><mn>180</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1568.gif" /></p></td></tr><tr><td align="left"><p>2.00–2.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4750</mn><mo>±</mo><mn>150</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1569.gif" /></p></td><td align="left"><p>0.7</p></td><td align="left"><p>1.3</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.2</p></td><td align="left"><p>1.2</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.2</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4100</mn><mo>±</mo><mn>130</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1570.gif" /></p></td></tr></tbody></table> </ephtml> </p> <p>Absolute and normalised differential cross-sections as functions of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>ℓ</mi></msubsup></math> </ephtml> (top) and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>η</mi><mi>ℓ</mi></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> (bottom). The columns show the bin ranges, measured cross-section and total uncertainty, relative statistical uncertainty, relative systematic uncertainties in various categories (see text), total relative uncertainty, and differential cross-section corrected to remove contributions via <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>W</mi><mo stretchy="false">→</mo><mi>τ</mi><mo stretchy="false">→</mo><mi>e</mi><mo stretchy="false">/</mo><mi>μ</mi></mrow></math> </ephtml> decays. Relative uncertainties smaller than 0.05% are indicated by '0.0'. The last bin includes overflows where indicated by the '+' sign</p> <p> <ephtml> <table frame="hsides" rules="groups"><thead><tr><th align="left"><p> Normalised</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mfrac><mn>1</mn><mi>σ</mi></mfrac><mi mathvariant="normal">d</mi><mi>σ</mi><mo stretchy="false">/</mo><mi mathvariant="normal">d</mi><mrow><mo stretchy="false">|</mo><msup><mi>η</mi><mi>ℓ</mi></msup><mo stretchy="false">|</mo></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1571.gif" /></p></th><th align="left"><p>Stat.</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1572.gif" /> mod.</p></th><th align="left"><p>Lept.</p></th><th align="left"><p>Jet/<italic>b</italic></p></th><th align="left"><p>Bkg.</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>L</mi><mo stretchy="false">/</mo><msub><mi>E</mi><mi mathvariant="normal">b</mi></msub></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1573.gif" /></p></th><th align="left"><p>Total</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mfrac><mn>1</mn><mi>σ</mi></mfrac><mi mathvariant="normal">d</mi><mi>σ</mi><mo stretchy="false">/</mo><mi mathvariant="normal">d</mi><mrow><mo stretchy="false">|</mo><msup><mi>η</mi><mi>ℓ</mi></msup><mo stretchy="false">|</mo></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1574.gif" /> (no <math xmlns="http://www.w3.org/1998/Math/MathML"><mi xmlns="">τ</mi></math><inline-graphic href="10052_2020_7907_Article_IEq1575.gif" />)</p></th></tr><tr><th align="left"><p>Bin (unit <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mo stretchy="false">|</mo><mi>η</mi><mo stretchy="false">|</mo></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1576.gif" />)</p></th><th align="left"><p>(<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msup><mn>10</mn><mrow><mo>-</mo><mn>1</mn></mrow></msup><mo stretchy="false">/</mo></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1577.gif" />unit <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mo stretchy="false">|</mo><mi>η</mi><mo stretchy="false">|</mo></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1578.gif" />)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msup><mn>10</mn><mrow><mo>-</mo><mn>1</mn></mrow></msup><mo stretchy="false">/</mo></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1579.gif" />unit <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mo stretchy="false">|</mo><mi>η</mi><mo stretchy="false">|</mo></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1580.gif" />)</p></th></tr></thead><tbody><tr><td align="left"><p>0.00–0.25</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>6.099</mn><mo>±</mo><mn>0.041</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1581.gif" /></p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>6.082</mn><mo>±</mo><mn>0.041</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1582.gif" /></p></td></tr><tr><td align="left"><p>0.25–0.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>5.832</mn><mo>±</mo><mn>0.035</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1583.gif" /></p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.6</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>5.816</mn><mo>±</mo><mn>0.035</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1584.gif" /></p></td></tr><tr><td align="left"><p>0.50–0.75</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>5.531</mn><mo>±</mo><mn>0.031</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1585.gif" /></p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.6</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>5.521</mn><mo>±</mo><mn>0.031</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1586.gif" /></p></td></tr><tr><td align="left"><p>0.75–1.00</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>5.056</mn><mo>±</mo><mn>0.028</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1587.gif" /></p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.6</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>5.049</mn><mo>±</mo><mn>0.028</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1588.gif" /></p></td></tr><tr><td align="left"><p>1.00–1.25</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4.472</mn><mo>±</mo><mn>0.027</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1589.gif" /></p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.6</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4.473</mn><mo>±</mo><mn>0.027</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1590.gif" /></p></td></tr><tr><td align="left"><p>1.25–1.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3.863</mn><mo>±</mo><mn>0.030</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1591.gif" /></p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3.863</mn><mo>±</mo><mn>0.030</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1592.gif" /></p></td></tr><tr><td align="left"><p>1.50–1.75</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3.211</mn><mo>±</mo><mn>0.028</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1593.gif" /></p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.9</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3.217</mn><mo>±</mo><mn>0.028</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1594.gif" /></p></td></tr><tr><td align="left"><p>1.75–2.00</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.584</mn><mo>±</mo><mn>0.027</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1595.gif" /></p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.0</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.599</mn><mo>±</mo><mn>0.027</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1596.gif" /></p></td></tr><tr><td align="left"><p>2.00–2.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.676</mn><mo>±</mo><mn>0.020</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1597.gif" /></p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.2</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.690</mn><mo>±</mo><mn>0.020</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1598.gif" /></p></td></tr></tbody></table> </ephtml> </p> <p>Absolute and normalised differential cross-sections as functions of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mrow><mi>e</mi><mi>μ</mi></mrow></msubsup></math> </ephtml> (top) and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></math> </ephtml> (bottom). The columns show the bin ranges, measured cross-section and total uncertainty, relative statistical uncertainty, relative systematic uncertainties in various categories (see text), total relative uncertainty, and differential cross-section corrected to remove contributions via <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>W</mi><mo stretchy="false">→</mo><mi>τ</mi><mo stretchy="false">→</mo><mi>e</mi><mo stretchy="false">/</mo><mi>μ</mi></mrow></math> </ephtml> decays. Relative uncertainties smaller than 0.05% are indicated by '0.0'. The last bin includes overflows where indicated by the '+' sign</p> <p> <ephtml> <table frame="hsides" rules="groups"><thead><tr><th align="left"><p>Absolute</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi mathvariant="normal">d</mi><mi>σ</mi><mo stretchy="false">/</mo><mi mathvariant="normal">d</mi><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mrow><mi>e</mi><mi>μ</mi></mrow></msubsup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1602.gif" /></p></th><th align="left"><p>Stat.</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1603.gif" /> mod.</p></th><th align="left"><p>Lept.</p></th><th align="left"><p>Jet/<italic>b</italic></p></th><th align="left"><p>Bkg.</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>L</mi><mo stretchy="false">/</mo><msub><mi>E</mi><mi mathvariant="normal">b</mi></msub></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1604.gif" /></p></th><th align="left"><p>Total</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi mathvariant="normal">d</mi><mi>σ</mi><mo stretchy="false">/</mo><mi mathvariant="normal">d</mi><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mrow><mi>e</mi><mi>μ</mi></mrow></msubsup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1605.gif" /> (no <math xmlns="http://www.w3.org/1998/Math/MathML"><mi xmlns="">τ</mi></math><inline-graphic href="10052_2020_7907_Article_IEq1606.gif" />)</p></th></tr><tr><th align="left"><p>Bin (<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1607.gif" />)</p></th><th align="left"><p>(fb/<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1608.gif" />)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(fb/<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1609.gif" />)</p></th></tr></thead><tbody><tr><td align="left"><p>0–20</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>45.1</mn><mo>±</mo><mn>1.4</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1610.gif" /></p></td><td align="left"><p>1.1</p></td><td align="left"><p>1.2</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.9</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.1</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>36.5</mn><mo>±</mo><mn>1.1</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1611.gif" /></p></td></tr><tr><td align="left"><p>20–40</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>110.1</mn><mo>±</mo><mn>3.1</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1612.gif" /></p></td><td align="left"><p>0.7</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.8</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.9</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>89.7</mn><mo>±</mo><mn>2.5</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1613.gif" /></p></td></tr><tr><td align="left"><p>40–60</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>159.8</mn><mo>±</mo><mn>4.5</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1614.gif" /></p></td><td align="left"><p>0.6</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.8</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>132.2</mn><mo>±</mo><mn>3.6</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1615.gif" /></p></td></tr><tr><td align="left"><p>60–80</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>156.2</mn><mo>±</mo><mn>4.3</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1616.gif" /></p></td><td align="left"><p>0.6</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.7</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>134.8</mn><mo>±</mo><mn>3.6</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1617.gif" /></p></td></tr><tr><td align="left"><p>80–100</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>110.1</mn><mo>±</mo><mn>3.1</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1618.gif" /></p></td><td align="left"><p>0.7</p></td><td align="left"><p>1.1</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.7</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>98.2</mn><mo>±</mo><mn>2.7</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1619.gif" /></p></td></tr><tr><td align="left"><p>100–120</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>62.6</mn><mo>±</mo><mn>1.9</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1620.gif" /></p></td><td align="left"><p>0.8</p></td><td align="left"><p>1.2</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.9</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.0</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>56.9</mn><mo>±</mo><mn>1.6</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1621.gif" /></p></td></tr><tr><td align="left"><p>120–150</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>26.67</mn><mo>±</mo><mn>0.90</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1622.gif" /></p></td><td align="left"><p>1.1</p></td><td align="left"><p>1.4</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.3</p></td><td align="left"><p>1.4</p></td><td align="left"><p>2.4</p></td><td align="left"><p>3.4</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>24.29</mn><mo>±</mo><mn>0.80</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1623.gif" /></p></td></tr><tr><td align="left"><p>150–200</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>7.15</mn><mo>±</mo><mn>0.35</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1624.gif" /></p></td><td align="left"><p>1.7</p></td><td align="left"><p>2.0</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.3</p></td><td align="left"><p>3.2</p></td><td align="left"><p>2.5</p></td><td align="left"><p>5.0</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>6.45</mn><mo>±</mo><mn>0.32</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1625.gif" /></p></td></tr><tr><td align="left"><p>200–300+</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.19</mn><mo>±</mo><mn>0.17</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1626.gif" /></p></td><td align="left"><p>3.2</p></td><td align="left"><p>3.4</p></td><td align="left"><p>1.5</p></td><td align="left"><p>0.6</p></td><td align="left"><p>13.2</p></td><td align="left"><p>2.8</p></td><td align="left"><p>14.3</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.06</mn><mo>±</mo><mn>0.15</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1627.gif" /></p></td></tr></tbody></table> </ephtml> </p> <p>Absolute and normalised differential cross-sections as functions of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mrow><mi>e</mi><mi>μ</mi></mrow></msubsup></math> </ephtml> (top) and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></math> </ephtml> (bottom). The columns show the bin ranges, measured cross-section and total uncertainty, relative statistical uncertainty, relative systematic uncertainties in various categories (see text), total relative uncertainty, and differential cross-section corrected to remove contributions via <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>W</mi><mo stretchy="false">→</mo><mi>τ</mi><mo stretchy="false">→</mo><mi>e</mi><mo stretchy="false">/</mo><mi>μ</mi></mrow></math> </ephtml> decays. Relative uncertainties smaller than 0.05% are indicated by '0.0'. The last bin includes overflows where indicated by the '+' sign</p> <p> <ephtml> <table frame="hsides" rules="groups"><thead><tr><th align="left"><p> Normalised</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mfrac><mn>1</mn><mi>σ</mi></mfrac><mi mathvariant="normal">d</mi><mi>σ</mi><mo stretchy="false">/</mo><mi mathvariant="normal">d</mi><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mrow><mi>e</mi><mi>μ</mi></mrow></msubsup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1628.gif" /></p></th><th align="left"><p>Stat.</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1629.gif" /> mod.</p></th><th align="left"><p>Lept.</p></th><th align="left"><p>Jet/<italic>b</italic></p></th><th align="left"><p>Bkg.</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>L</mi><mo stretchy="false">/</mo><msub><mi>E</mi><mi mathvariant="normal">b</mi></msub></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1630.gif" /></p></th><th align="left"><p>Total</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mfrac><mn>1</mn><mi>σ</mi></mfrac><mi mathvariant="normal">d</mi><mi>σ</mi><mo stretchy="false">/</mo><mi mathvariant="normal">d</mi><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mrow><mi>e</mi><mi>μ</mi></mrow></msubsup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1631.gif" /> (no <math xmlns="http://www.w3.org/1998/Math/MathML"><mi xmlns="">τ</mi></math><inline-graphic href="10052_2020_7907_Article_IEq1632.gif" />)</p></th></tr><tr><th align="left"><p>Bin (<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1633.gif" />)</p></th><th align="left"><p>(<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msup><mn>10</mn><mrow><mo>-</mo><mn>2</mn></mrow></msup><mo stretchy="false">/</mo></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1634.gif" /><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1635.gif" />)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msup><mn>10</mn><mrow><mo>-</mo><mn>2</mn></mrow></msup><mo stretchy="false">/</mo></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1636.gif" /><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1637.gif" />)</p></th></tr></thead><tbody><tr><td align="left"><p>0–20</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.3189</mn><mo>±</mo><mn>0.0051</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1638.gif" /></p></td><td align="left"><p>1.1</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.6</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.3011</mn><mo>±</mo><mn>0.0049</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1639.gif" /></p></td></tr><tr><td align="left"><p>20–40</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.7776</mn><mo>±</mo><mn>0.0082</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1640.gif" /></p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.1</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.7402</mn><mo>±</mo><mn>0.0081</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1641.gif" /></p></td></tr><tr><td align="left"><p>40–60</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.1286</mn><mo>±</mo><mn>0.0088</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1642.gif" /></p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.0905</mn><mo>±</mo><mn>0.0089</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1643.gif" /></p></td></tr><tr><td align="left"><p>60–80</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.1035</mn><mo>±</mo><mn>0.0070</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1644.gif" /></p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.6</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.1121</mn><mo>±</mo><mn>0.0072</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1645.gif" /></p></td></tr><tr><td align="left"><p>80–100</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.7780</mn><mo>±</mo><mn>0.0058</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1646.gif" /></p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.8098</mn><mo>±</mo><mn>0.0059</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1647.gif" /></p></td></tr><tr><td align="left"><p>100–120</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.4425</mn><mo>±</mo><mn>0.0051</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1648.gif" /></p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.2</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.4694</mn><mo>±</mo><mn>0.0054</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1649.gif" /></p></td></tr><tr><td align="left"><p>120–150</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.1884</mn><mo>±</mo><mn>0.0035</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1650.gif" /></p></td><td align="left"><p>1.0</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.2</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.1</p></td><td align="left"><p>1.9</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.2003</mn><mo>±</mo><mn>0.0038</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1651.gif" /></p></td></tr><tr><td align="left"><p>150–200</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.0505</mn><mo>±</mo><mn>0.0020</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1652.gif" /></p></td><td align="left"><p>1.7</p></td><td align="left"><p>1.8</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.3</p></td><td align="left"><p>2.9</p></td><td align="left"><p>0.2</p></td><td align="left"><p>4.0</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.0532</mn><mo>±</mo><mn>0.0021</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1653.gif" /></p></td></tr><tr><td align="left"><p>200–300+</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.0084</mn><mo>±</mo><mn>0.0012</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1654.gif" /></p></td><td align="left"><p>3.2</p></td><td align="left"><p>3.4</p></td><td align="left"><p>1.5</p></td><td align="left"><p>0.5</p></td><td align="left"><p>13.0</p></td><td align="left"><p>0.5</p></td><td align="left"><p>13.9</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.0087</mn><mo>±</mo><mn>0.0012</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1655.gif" /></p></td></tr></tbody></table> </ephtml> </p> <p>Absolute and normalised differential cross-sections as functions of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mrow><mi>e</mi><mi>μ</mi></mrow></msubsup></math> </ephtml> (top) and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></math> </ephtml> (bottom). The columns show the bin ranges, measured cross-section and total uncertainty, relative statistical uncertainty, relative systematic uncertainties in various categories (see text), total relative uncertainty, and differential cross-section corrected to remove contributions via <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>W</mi><mo stretchy="false">→</mo><mi>τ</mi><mo stretchy="false">→</mo><mi>e</mi><mo stretchy="false">/</mo><mi>μ</mi></mrow></math> </ephtml> decays. Relative uncertainties smaller than 0.05% are indicated by '0.0'. The last bin includes overflows where indicated by the '+' sign</p> <p> <ephtml> <table frame="hsides" rules="groups"><thead><tr><th align="left"><p> Absolute</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi mathvariant="normal">d</mi><mi>σ</mi><mo stretchy="false">/</mo><mi mathvariant="normal">d</mi><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1656.gif" /></p></th><th align="left"><p>Stat.</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1657.gif" /> mod.</p></th><th align="left"><p>Lept.</p></th><th align="left"><p>Jet/<italic>b</italic></p></th><th align="left"><p>Bkg.</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>L</mi><mo stretchy="false">/</mo><msub><mi>E</mi><mi mathvariant="normal">b</mi></msub></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1658.gif" /></p></th><th align="left"><p>Total</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi mathvariant="normal">d</mi><mi>σ</mi><mo stretchy="false">/</mo><mi mathvariant="normal">d</mi><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1659.gif" /> (no <math xmlns="http://www.w3.org/1998/Math/MathML"><mi xmlns="">τ</mi></math><inline-graphic href="10052_2020_7907_Article_IEq1660.gif" />)</p></th></tr><tr><th align="left"><p>Bin (<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1661.gif" />)</p></th><th align="left"><p>(fb/<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1662.gif" />)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(fb/<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1663.gif" />)</p></th></tr></thead><tbody><tr><td align="left"><p>0–20</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>19.98</mn><mo>±</mo><mn>0.74</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1664.gif" /></p></td><td align="left"><p>2.0</p></td><td align="left"><p>1.3</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.3</p></td><td align="left"><p>1.2</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>16.57</mn><mo>±</mo><mn>0.60</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1665.gif" /></p></td></tr><tr><td align="left"><p>20–40</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>54.3</mn><mo>±</mo><mn>1.6</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1666.gif" /></p></td><td align="left"><p>1.0</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.2</p></td><td align="left"><p>1.0</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.0</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>45.6</mn><mo>±</mo><mn>1.3</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1667.gif" /></p></td></tr><tr><td align="left"><p>40–60</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>88.2</mn><mo>±</mo><mn>2.6</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1668.gif" /></p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.2</p></td><td align="left"><p>1.0</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.9</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>73.1</mn><mo>±</mo><mn>2.1</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1669.gif" /></p></td></tr><tr><td align="left"><p>60–80</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>107.0</mn><mo>±</mo><mn>3.0</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1670.gif" /></p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.9</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>88.9</mn><mo>±</mo><mn>2.4</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1671.gif" /></p></td></tr><tr><td align="left"><p>80–100</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>102.3</mn><mo>±</mo><mn>2.9</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1672.gif" /></p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.8</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>86.4</mn><mo>±</mo><mn>2.4</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1673.gif" /></p></td></tr><tr><td align="left"><p>100–120</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>83.8</mn><mo>±</mo><mn>2.3</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1674.gif" /></p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.7</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>71.7</mn><mo>±</mo><mn>2.0</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1675.gif" /></p></td></tr><tr><td align="left"><p>120–150</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>59.8</mn><mo>±</mo><mn>1.7</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1676.gif" /></p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.7</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>51.9</mn><mo>±</mo><mn>1.4</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1677.gif" /></p></td></tr><tr><td align="left"><p>150–200</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>33.80</mn><mo>±</mo><mn>0.97</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1678.gif" /></p></td><td align="left"><p>0.7</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.9</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.9</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>29.96</mn><mo>±</mo><mn>0.84</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1679.gif" /></p></td></tr><tr><td align="left"><p>200–250</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>15.75</mn><mo>±</mo><mn>0.51</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1680.gif" /></p></td><td align="left"><p>1.1</p></td><td align="left"><p>1.2</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.4</p></td><td align="left"><p>1.3</p></td><td align="left"><p>2.4</p></td><td align="left"><p>3.2</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>14.21</mn><mo>±</mo><mn>0.45</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1681.gif" /></p></td></tr><tr><td align="left"><p>250–300</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>7.51</mn><mo>±</mo><mn>0.29</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1682.gif" /></p></td><td align="left"><p>1.6</p></td><td align="left"><p>1.5</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.2</p></td><td align="left"><p>1.8</p></td><td align="left"><p>2.4</p></td><td align="left"><p>3.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>6.85</mn><mo>±</mo><mn>0.25</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1683.gif" /></p></td></tr><tr><td align="left"><p>300–400</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.84</mn><mo>±</mo><mn>0.13</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1684.gif" /></p></td><td align="left"><p>1.8</p></td><td align="left"><p>2.0</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.2</p></td><td align="left"><p>2.7</p></td><td align="left"><p>2.4</p></td><td align="left"><p>4.5</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.62</mn><mo>±</mo><mn>0.11</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1685.gif" /></p></td></tr><tr><td align="left"><p>400–500+</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.48</mn><mo>±</mo><mn>0.09</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1686.gif" /></p></td><td align="left"><p>2.7</p></td><td align="left"><p>2.7</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.3</p></td><td align="left"><p>3.7</p></td><td align="left"><p>2.4</p></td><td align="left"><p>5.9</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.38</mn><mo>±</mo><mn>0.08</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1687.gif" /></p></td></tr></tbody></table> </ephtml> </p> <p>Absolute and normalised differential cross-sections as functions of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mrow><mi>e</mi><mi>μ</mi></mrow></msubsup></math> </ephtml> (top) and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></math> </ephtml> (bottom). The columns show the bin ranges, measured cross-section and total uncertainty, relative statistical uncertainty, relative systematic uncertainties in various categories (see text), total relative uncertainty, and differential cross-section corrected to remove contributions via <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>W</mi><mo stretchy="false">→</mo><mi>τ</mi><mo stretchy="false">→</mo><mi>e</mi><mo stretchy="false">/</mo><mi>μ</mi></mrow></math> </ephtml> decays. Relative uncertainties smaller than 0.05% are indicated by '0.0'. The last bin includes overflows where indicated by the '+' sign</p> <p> <ephtml> <table frame="hsides" rules="groups"><thead><tr><th align="left"><p> Normalised</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mfrac><mn>1</mn><mi>σ</mi></mfrac><mi mathvariant="normal">d</mi><mi>σ</mi><mo stretchy="false">/</mo><mi mathvariant="normal">d</mi><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1688.gif" /></p></th><th align="left"><p>Stat.</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1689.gif" /> mod.</p></th><th align="left"><p>Lept.</p></th><th align="left"><p>Jet/<italic>b</italic></p></th><th align="left"><p>Bkg.</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>L</mi><mo stretchy="false">/</mo><msub><mi>E</mi><mi mathvariant="normal">b</mi></msub></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1690.gif" /></p></th><th align="left"><p>Total</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mfrac><mn>1</mn><mi>σ</mi></mfrac><mi mathvariant="normal">d</mi><mi>σ</mi><mo stretchy="false">/</mo><mi mathvariant="normal">d</mi><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1691.gif" /> (no <math xmlns="http://www.w3.org/1998/Math/MathML"><mi xmlns="">τ</mi></math><inline-graphic href="10052_2020_7907_Article_IEq1692.gif" />)</p></th></tr><tr><th align="left"><p>Bin (<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1693.gif" />)</p></th><th align="left"><p>(<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msup><mn>10</mn><mrow><mo>-</mo><mn>3</mn></mrow></msup><mo stretchy="false">/</mo></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1694.gif" /><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1695.gif" />)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msup><mn>10</mn><mrow><mo>-</mo><mn>3</mn></mrow></msup><mo stretchy="false">/</mo></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1696.gif" /><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1697.gif" />)</p></th></tr></thead><tbody><tr><td align="left"><p>0–20</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.408</mn><mo>±</mo><mn>0.036</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1698.gif" /></p></td><td align="left"><p>2.0</p></td><td align="left"><p>1.1</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.2</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.0</p></td><td align="left"><p>2.5</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.364</mn><mo>±</mo><mn>0.034</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1699.gif" /></p></td></tr><tr><td align="left"><p>20–40</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3.826</mn><mo>±</mo><mn>0.055</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1700.gif" /></p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.4</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3.751</mn><mo>±</mo><mn>0.053</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1701.gif" /></p></td></tr><tr><td align="left"><p>40–60</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>6.218</mn><mo>±</mo><mn>0.073</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1702.gif" /></p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.2</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>6.017</mn><mo>±</mo><mn>0.069</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1703.gif" /></p></td></tr><tr><td align="left"><p>60–80</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>7.541</mn><mo>±</mo><mn>0.068</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1704.gif" /></p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.9</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>7.315</mn><mo>±</mo><mn>0.066</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1705.gif" /></p></td></tr><tr><td align="left"><p>80–100</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>7.210</mn><mo>±</mo><mn>0.061</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1706.gif" /></p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>7.108</mn><mo>±</mo><mn>0.060</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1707.gif" /></p></td></tr><tr><td align="left"><p>100–120</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>5.907</mn><mo>±</mo><mn>0.049</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1708.gif" /></p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>5.898</mn><mo>±</mo><mn>0.049</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1709.gif" /></p></td></tr><tr><td align="left"><p>120–150</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4.212</mn><mo>±</mo><mn>0.033</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1710.gif" /></p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4.270</mn><mo>±</mo><mn>0.034</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1711.gif" /></p></td></tr><tr><td align="left"><p>150–200</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.382</mn><mo>±</mo><mn>0.025</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1712.gif" /></p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.0</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.466</mn><mo>±</mo><mn>0.024</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1713.gif" /></p></td></tr><tr><td align="left"><p>200–250</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.110</mn><mo>±</mo><mn>0.019</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1714.gif" /></p></td><td align="left"><p>1.1</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.2</p></td><td align="left"><p>1.1</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.169</mn><mo>±</mo><mn>0.019</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1715.gif" /></p></td></tr><tr><td align="left"><p>250–300</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.529</mn><mo>±</mo><mn>0.014</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1716.gif" /></p></td><td align="left"><p>1.6</p></td><td align="left"><p>1.2</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.1</p></td><td align="left"><p>1.6</p></td><td align="left"><p>0.1</p></td><td align="left"><p>2.6</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.564</mn><mo>±</mo><mn>0.014</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1717.gif" /></p></td></tr><tr><td align="left"><p>300–400</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.2000</mn><mo>±</mo><mn>0.0071</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1718.gif" /></p></td><td align="left"><p>1.8</p></td><td align="left"><p>1.6</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.1</p></td><td align="left"><p>2.6</p></td><td align="left"><p>0.1</p></td><td align="left"><p>3.6</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.2154</mn><mo>±</mo><mn>0.0073</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1719.gif" /></p></td></tr><tr><td align="left"><p>400–500+</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.1041</mn><mo>±</mo><mn>0.0053</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1720.gif" /></p></td><td align="left"><p>2.7</p></td><td align="left"><p>2.4</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.2</p></td><td align="left"><p>3.5</p></td><td align="left"><p>0.1</p></td><td align="left"><p>5.1</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.1132</mn><mo>±</mo><mn>0.0055</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1721.gif" /></p></td></tr></tbody></table> </ephtml> </p> <p>Absolute and normalised differential cross-sections as functions of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>y</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> (top) and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi mathvariant="normal">Δ</mi><msup><mi>ϕ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math> </ephtml> (bottom). The columns show the bin ranges, measured cross-section and total uncertainty, relative statistical uncertainty, relative systematic uncertainties in various categories (see text), total relative uncertainty, and differential cross-section corrected to remove contributions via <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>W</mi><mo stretchy="false">→</mo><mi>τ</mi><mo stretchy="false">→</mo><mi>e</mi><mo stretchy="false">/</mo><mi>μ</mi></mrow></math> </ephtml> decays. Relative uncertainties smaller than 0.05% are indicated by '0.0'. The bin boundaries for <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi mathvariant="normal">Δ</mi><msup><mi>ϕ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math> </ephtml> correspond to exact multiples of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>π</mi><mo stretchy="false">/</mo><mn>10</mn></mrow></math> </ephtml> but are quoted to two decimal places</p> <p> <ephtml> <table frame="hsides" rules="groups"><thead><tr><th align="left"><p>Absolute</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mrow><mi mathvariant="normal">d</mi><mi>σ</mi><mo stretchy="false">/</mo><mi mathvariant="normal">d</mi><mo stretchy="false">|</mo></mrow><msup><mi>y</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1727.gif" /></p></th><th align="left"><p>Stat.</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1728.gif" /> mod.</p></th><th align="left"><p>Lept.</p></th><th align="left"><p>Jet/<italic>b</italic></p></th><th align="left"><p>Bkg.</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>L</mi><mo stretchy="false">/</mo><msub><mi>E</mi><mi mathvariant="normal">b</mi></msub></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1729.gif" /></p></th><th align="left"><p>Total</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mrow><mi mathvariant="normal">d</mi><mi>σ</mi><mo stretchy="false">/</mo><mi mathvariant="normal">d</mi><mo stretchy="false">|</mo></mrow><msup><mi>y</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1730.gif" /> (no <math xmlns="http://www.w3.org/1998/Math/MathML"><mi xmlns="">τ</mi></math><inline-graphic href="10052_2020_7907_Article_IEq1731.gif" />)</p></th></tr><tr><th align="left"><p>Bin (unit |<italic>y</italic>|)</p></th><th align="left"><p>(fb/unit |<italic>y</italic>|)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(fb/unit |<italic>y</italic>|)</p></th></tr></thead><tbody><tr><td align="left"><p>0.00–0.25</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>10700</mn><mo>±</mo><mn>290</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1732.gif" /></p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.7</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>9150</mn><mo>±</mo><mn>240</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1733.gif" /></p></td></tr><tr><td align="left"><p>0.25–0.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>10160</mn><mo>±</mo><mn>270</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1734.gif" /></p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.7</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>8700</mn><mo>±</mo><mn>230</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1735.gif" /></p></td></tr><tr><td align="left"><p>0.50–0.75</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>9300</mn><mo>±</mo><mn>260</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1736.gif" /></p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.7</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>7970</mn><mo>±</mo><mn>210</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1737.gif" /></p></td></tr><tr><td align="left"><p>0.75–1.00</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>8140</mn><mo>±</mo><mn>230</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1738.gif" /></p></td><td align="left"><p>0.7</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.8</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>6970</mn><mo>±</mo><mn>190</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1739.gif" /></p></td></tr><tr><td align="left"><p>1.00–1.25</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>6620</mn><mo>±</mo><mn>190</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1740.gif" /></p></td><td align="left"><p>0.8</p></td><td align="left"><p>1.1</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.8</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.9</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>5680</mn><mo>±</mo><mn>160</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1741.gif" /></p></td></tr><tr><td align="left"><p>1.25–1.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>5030</mn><mo>±</mo><mn>150</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1742.gif" /></p></td><td align="left"><p>1.0</p></td><td align="left"><p>1.2</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.9</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.0</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4320</mn><mo>±</mo><mn>130</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1743.gif" /></p></td></tr><tr><td align="left"><p>1.50–1.75</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3460</mn><mo>±</mo><mn>110</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1744.gif" /></p></td><td align="left"><p>1.2</p></td><td align="left"><p>1.4</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.2</p></td><td align="left"><p>1.1</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.3</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2969</mn><mo>±</mo><mn>96</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1745.gif" /></p></td></tr><tr><td align="left"><p>1.75–2.00</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2085</mn><mo>±</mo><mn>76</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1746.gif" /></p></td><td align="left"><p>1.7</p></td><td align="left"><p>1.6</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.2</p></td><td align="left"><p>1.3</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1790</mn><mo>±</mo><mn>65</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1747.gif" /></p></td></tr><tr><td align="left"><p>2.00–2.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>545</mn><mo>±</mo><mn>26</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1748.gif" /></p></td><td align="left"><p>2.6</p></td><td align="left"><p>2.1</p></td><td align="left"><p>1.1</p></td><td align="left"><p>0.3</p></td><td align="left"><p>2.2</p></td><td align="left"><p>2.4</p></td><td align="left"><p>4.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>467</mn><mo>±</mo><mn>22</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1749.gif" /></p></td></tr></tbody></table> </ephtml> </p> <p>Absolute and normalised differential cross-sections as functions of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>y</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> (top) and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi mathvariant="normal">Δ</mi><msup><mi>ϕ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math> </ephtml> (bottom). The columns show the bin ranges, measured cross-section and total uncertainty, relative statistical uncertainty, relative systematic uncertainties in various categories (see text), total relative uncertainty, and differential cross-section corrected to remove contributions via <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>W</mi><mo stretchy="false">→</mo><mi>τ</mi><mo stretchy="false">→</mo><mi>e</mi><mo stretchy="false">/</mo><mi>μ</mi></mrow></math> </ephtml> decays. Relative uncertainties smaller than 0.05% are indicated by '0.0'. The bin boundaries for <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi mathvariant="normal">Δ</mi><msup><mi>ϕ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math> </ephtml> correspond to exact multiples of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>π</mi><mo stretchy="false">/</mo><mn>10</mn></mrow></math> </ephtml> but are quoted to two decimal places</p> <p> <ephtml> <table frame="hsides" rules="groups"><thead><tr><th align="left"><p> Normalised</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mfrac><mn>1</mn><mi>σ</mi></mfrac><mi mathvariant="normal">d</mi><mi>σ</mi><mo stretchy="false">/</mo><mi mathvariant="normal">d</mi><mrow><mo stretchy="false">|</mo><msup><mi>y</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mo stretchy="false">|</mo></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1750.gif" /></p></th><th align="left"><p>Stat.</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1751.gif" /> mod.</p></th><th align="left"><p>Lept.</p></th><th align="left"><p>Jet/<italic>b</italic></p></th><th align="left"><p>Bkg.</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>L</mi><mo stretchy="false">/</mo><msub><mi>E</mi><mi mathvariant="normal">b</mi></msub></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1752.gif" /></p></th><th align="left"><p>Total</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mfrac><mn>1</mn><mi>σ</mi></mfrac><mi mathvariant="normal">d</mi><mi>σ</mi><mo stretchy="false">/</mo><mi mathvariant="normal">d</mi><mrow><mo stretchy="false">|</mo><msup><mi>y</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mo stretchy="false">|</mo></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1753.gif" /> (no <math xmlns="http://www.w3.org/1998/Math/MathML"><mi xmlns="">τ</mi></math><inline-graphic href="10052_2020_7907_Article_IEq1754.gif" />)</p></th></tr><tr><th align="left"><p>Bin (unit |<italic>y</italic>|)</p></th><th align="left"><p>(<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msup><mn>10</mn><mrow><mo>-</mo><mn>1</mn></mrow></msup><mo stretchy="false">/</mo></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1755.gif" />unit |<italic>y</italic>|)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msup><mn>10</mn><mrow><mo>-</mo><mn>1</mn></mrow></msup><mo stretchy="false">/</mo></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1756.gif" />unit |<italic>y</italic>|)</p></th></tr></thead><tbody><tr><td align="left"><p>0.00–0.25</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>7.560</mn><mo>±</mo><mn>0.056</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1757.gif" /></p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>7.550</mn><mo>±</mo><mn>0.056</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1758.gif" /></p></td></tr><tr><td align="left"><p>0.25–0.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>7.184</mn><mo>±</mo><mn>0.050</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1759.gif" /></p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>7.182</mn><mo>±</mo><mn>0.050</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1760.gif" /></p></td></tr><tr><td align="left"><p>0.50–0.75</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>6.574</mn><mo>±</mo><mn>0.045</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1761.gif" /></p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>6.574</mn><mo>±</mo><mn>0.045</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1762.gif" /></p></td></tr><tr><td align="left"><p>0.75–1.00</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>5.752</mn><mo>±</mo><mn>0.042</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1763.gif" /></p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>5.748</mn><mo>±</mo><mn>0.043</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1764.gif" /></p></td></tr><tr><td align="left"><p>1.00–1.25</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4.679</mn><mo>±</mo><mn>0.041</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1765.gif" /></p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.9</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4.688</mn><mo>±</mo><mn>0.041</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1766.gif" /></p></td></tr><tr><td align="left"><p>1.25–1.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3.558</mn><mo>±</mo><mn>0.040</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1767.gif" /></p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.1</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3.562</mn><mo>±</mo><mn>0.040</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1768.gif" /></p></td></tr><tr><td align="left"><p>1.50–1.75</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.449</mn><mo>±</mo><mn>0.037</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1769.gif" /></p></td><td align="left"><p>1.2</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.5</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.449</mn><mo>±</mo><mn>0.037</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1770.gif" /></p></td></tr><tr><td align="left"><p>1.75–2.00</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.474</mn><mo>±</mo><mn>0.031</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1771.gif" /></p></td><td align="left"><p>1.7</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.0</p></td><td align="left"><p>2.1</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.477</mn><mo>±</mo><mn>0.032</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1772.gif" /></p></td></tr><tr><td align="left"><p>2.00–2.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.385</mn><mo>±</mo><mn>0.013</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1773.gif" /></p></td><td align="left"><p>2.6</p></td><td align="left"><p>1.4</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.1</p></td><td align="left"><p>1.8</p></td><td align="left"><p>0.1</p></td><td align="left"><p>3.5</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.386</mn><mo>±</mo><mn>0.014</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1774.gif" /></p></td></tr></tbody></table> </ephtml> </p> <p>Absolute and normalised differential cross-sections as functions of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>y</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> (top) and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi mathvariant="normal">Δ</mi><msup><mi>ϕ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math> </ephtml> (bottom). The columns show the bin ranges, measured cross-section and total uncertainty, relative statistical uncertainty, relative systematic uncertainties in various categories (see text), total relative uncertainty, and differential cross-section corrected to remove contributions via <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>W</mi><mo stretchy="false">→</mo><mi>τ</mi><mo stretchy="false">→</mo><mi>e</mi><mo stretchy="false">/</mo><mi>μ</mi></mrow></math> </ephtml> decays. Relative uncertainties smaller than 0.05% are indicated by '0.0'. The bin boundaries for <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi mathvariant="normal">Δ</mi><msup><mi>ϕ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math> </ephtml> correspond to exact multiples of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>π</mi><mo stretchy="false">/</mo><mn>10</mn></mrow></math> </ephtml> but are quoted to two decimal places</p> <p> <ephtml> <table frame="hsides" rules="groups"><thead><tr><th align="left"><p> Absolute</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi mathvariant="normal">d</mi><mi>σ</mi><mo stretchy="false">/</mo><mi mathvariant="normal">d</mi><mi mathvariant="normal">Δ</mi><msup><mi>ϕ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1775.gif" /></p></th><th align="left"><p>Stat.</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1776.gif" /> mod.</p></th><th align="left"><p>Lept.</p></th><th align="left"><p>Jet/<italic>b</italic></p></th><th align="left"><p>Bkg.</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>L</mi><mo stretchy="false">/</mo><msub><mi>E</mi><mi mathvariant="normal">b</mi></msub></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1777.gif" /></p></th><th align="left"><p>Total</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi mathvariant="normal">d</mi><mi>σ</mi><mo stretchy="false">/</mo><mi mathvariant="normal">d</mi><mi mathvariant="normal">Δ</mi><msup><mi>ϕ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1778.gif" /> (no <math xmlns="http://www.w3.org/1998/Math/MathML"><mi xmlns="">τ</mi></math><inline-graphic href="10052_2020_7907_Article_IEq1779.gif" />)</p></th></tr><tr><th align="left"><p>Bin (rad)</p></th><th align="left"><p>(fb/rad)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(fb/rad)</p></th></tr></thead><tbody><tr><td align="left"><p>0.00–0.31</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3250</mn><mo>±</mo><mn>110</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1780.gif" /></p></td><td align="left"><p>1.1</p></td><td align="left"><p>2.0</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.8</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.4</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2847</mn><mo>±</mo><mn>90</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1781.gif" /></p></td></tr><tr><td align="left"><p>0.31–0.63</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3280</mn><mo>±</mo><mn>110</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1782.gif" /></p></td><td align="left"><p>1.0</p></td><td align="left"><p>1.7</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.8</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.2</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2882</mn><mo>±</mo><mn>87</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1783.gif" /></p></td></tr><tr><td align="left"><p>0.63–0.94</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3370</mn><mo>±</mo><mn>100</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1784.gif" /></p></td><td align="left"><p>1.0</p></td><td align="left"><p>1.4</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.8</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.1</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2965</mn><mo>±</mo><mn>88</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1785.gif" /></p></td></tr><tr><td align="left"><p>0.94–1.26</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3680</mn><mo>±</mo><mn>110</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1786.gif" /></p></td><td align="left"><p>0.9</p></td><td align="left"><p>1.2</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.8</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.0</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3219</mn><mo>±</mo><mn>93</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1787.gif" /></p></td></tr><tr><td align="left"><p>1.26–1.57</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4000</mn><mo>±</mo><mn>120</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1788.gif" /></p></td><td align="left"><p>0.9</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.8</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.9</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3476</mn><mo>±</mo><mn>98</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1789.gif" /></p></td></tr><tr><td align="left"><p>1.57–1.88</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4460</mn><mo>±</mo><mn>130</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1790.gif" /></p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.8</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3850</mn><mo>±</mo><mn>110</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1791.gif" /></p></td></tr><tr><td align="left"><p>1.88–2.20</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4980</mn><mo>±</mo><mn>140</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1792.gif" /></p></td><td align="left"><p>0.8</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.8</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4260</mn><mo>±</mo><mn>120</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1793.gif" /></p></td></tr><tr><td align="left"><p>2.20–2.51</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>5610</mn><mo>±</mo><mn>160</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1794.gif" /></p></td><td align="left"><p>0.7</p></td><td align="left"><p>1.1</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.7</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.9</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4740</mn><mo>±</mo><mn>130</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1795.gif" /></p></td></tr><tr><td align="left"><p>2.51–2.83</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>6030</mn><mo>±</mo><mn>180</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1796.gif" /></p></td><td align="left"><p>0.7</p></td><td align="left"><p>1.3</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.8</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.0</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>5060</mn><mo>±</mo><mn>150</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1797.gif" /></p></td></tr><tr><td align="left"><p>2.83–3.14</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>6420</mn><mo>±</mo><mn>200</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1798.gif" /></p></td><td align="left"><p>0.7</p></td><td align="left"><p>1.6</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.8</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.1</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>5350</mn><mo>±</mo><mn>170</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1799.gif" /></p></td></tr></tbody></table> </ephtml> </p> <p>Absolute and normalised differential cross-sections as functions of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>y</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mrow><mo stretchy="false">|</mo></mrow></mrow></math> </ephtml> (top) and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi mathvariant="normal">Δ</mi><msup><mi>ϕ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math> </ephtml> (bottom). The columns show the bin ranges, measured cross-section and total uncertainty, relative statistical uncertainty, relative systematic uncertainties in various categories (see text), total relative uncertainty, and differential cross-section corrected to remove contributions via <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>W</mi><mo stretchy="false">→</mo><mi>τ</mi><mo stretchy="false">→</mo><mi>e</mi><mo stretchy="false">/</mo><mi>μ</mi></mrow></math> </ephtml> decays. Relative uncertainties smaller than 0.05% are indicated by '0.0'. The bin boundaries for <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi mathvariant="normal">Δ</mi><msup><mi>ϕ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math> </ephtml> correspond to exact multiples of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>π</mi><mo stretchy="false">/</mo><mn>10</mn></mrow></math> </ephtml> but are quoted to two decimal places</p> <p> <ephtml> <table frame="hsides" rules="groups"><thead><tr><th align="left"><p> Normalised</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mfrac><mn>1</mn><mi>σ</mi></mfrac><mi mathvariant="normal">d</mi><mi>σ</mi><mo stretchy="false">/</mo><mi mathvariant="normal">d</mi><mi mathvariant="normal">Δ</mi><msup><mi>ϕ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1800.gif" /></p></th><th align="left"><p>Stat.</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1801.gif" /> mod.</p></th><th align="left"><p>Lept.</p></th><th align="left"><p>Jet/<italic>b</italic></p></th><th align="left"><p>Bkg.</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>L</mi><mo stretchy="false">/</mo><msub><mi>E</mi><mi mathvariant="normal">b</mi></msub></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1802.gif" /></p></th><th align="left"><p>Total</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mfrac><mn>1</mn><mi>σ</mi></mfrac><mi mathvariant="normal">d</mi><mi>σ</mi><mo stretchy="false">/</mo><mi mathvariant="normal">d</mi><mi mathvariant="normal">Δ</mi><msup><mi>ϕ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1803.gif" /> (no <math xmlns="http://www.w3.org/1998/Math/MathML"><mi xmlns="">τ</mi></math><inline-graphic href="10052_2020_7907_Article_IEq1804.gif" />)</p></th></tr><tr><th align="left"><p>Bin (rad)</p></th><th align="left"><p>[<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msup><mn>10</mn><mrow><mo>-</mo><mn>1</mn></mrow></msup><mo stretchy="false">/</mo></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1805.gif" />rad]</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msup><mn>10</mn><mrow><mo>-</mo><mn>1</mn></mrow></msup><mo stretchy="false">/</mo></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1806.gif" />rad)</p></th></tr></thead><tbody><tr><td align="left"><p>0.00–0.31</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.298</mn><mo>±</mo><mn>0.050</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1807.gif" /></p></td><td align="left"><p>1.0</p></td><td align="left"><p>1.9</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.0</p></td><td align="left"><p>2.2</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.345</mn><mo>±</mo><mn>0.044</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1808.gif" /></p></td></tr><tr><td align="left"><p>0.31–0.63</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.316</mn><mo>±</mo><mn>0.043</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1809.gif" /></p></td><td align="left"><p>0.9</p></td><td align="left"><p>1.5</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.374</mn><mo>±</mo><mn>0.040</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1810.gif" /></p></td></tr><tr><td align="left"><p>0.63–0.94</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.380</mn><mo>±</mo><mn>0.037</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1811.gif" /></p></td><td align="left"><p>0.9</p></td><td align="left"><p>1.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.6</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.442</mn><mo>±</mo><mn>0.036</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1812.gif" /></p></td></tr><tr><td align="left"><p>0.94–1.26</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.600</mn><mo>±</mo><mn>0.033</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1813.gif" /></p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.3</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.651</mn><mo>±</mo><mn>0.034</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1814.gif" /></p></td></tr><tr><td align="left"><p>1.26–1.57</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.823</mn><mo>±</mo><mn>0.029</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1815.gif" /></p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.0</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.864</mn><mo>±</mo><mn>0.031</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1816.gif" /></p></td></tr><tr><td align="left"><p>1.57–1.88</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3.149</mn><mo>±</mo><mn>0.028</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1817.gif" /></p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.9</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3.172</mn><mo>±</mo><mn>0.029</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1818.gif" /></p></td></tr><tr><td align="left"><p>1.88–2.20</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3.516</mn><mo>±</mo><mn>0.031</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1819.gif" /></p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.9</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3.505</mn><mo>±</mo><mn>0.030</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1820.gif" /></p></td></tr><tr><td align="left"><p>2.20–2.51</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3.960</mn><mo>±</mo><mn>0.040</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1821.gif" /></p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.0</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3.908</mn><mo>±</mo><mn>0.038</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1822.gif" /></p></td></tr><tr><td align="left"><p>2.51–2.83</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4.255</mn><mo>±</mo><mn>0.054</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1823.gif" /></p></td><td align="left"><p>0.7</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.3</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4.164</mn><mo>±</mo><mn>0.052</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1824.gif" /></p></td></tr><tr><td align="left"><p>2.83–3.14</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4.533</mn><mo>±</mo><mn>0.070</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1825.gif" /></p></td><td align="left"><p>0.7</p></td><td align="left"><p>1.4</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.6</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4.405</mn><mo>±</mo><mn>0.071</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1826.gif" /></p></td></tr></tbody></table> </ephtml> </p> <p>Absolute and normalised differential cross-sections as functions of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>e</mi></msubsup><mo>+</mo><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>μ</mi></msubsup></mrow></math> </ephtml> (top) and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msup><mi>E</mi><mi>e</mi></msup><mo>+</mo><msup><mi>E</mi><mi>μ</mi></msup></mrow></math> </ephtml> (bottom). The columns show the bin ranges, measured cross-section and total uncertainty, relative statistical uncertainty, relative systematic uncertainties in various categories (see text), total relative uncertainty, and differential cross-section corrected to remove contributions via <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>W</mi><mo stretchy="false">→</mo><mi>τ</mi><mo stretchy="false">→</mo><mi>e</mi><mo stretchy="false">/</mo><mi>μ</mi></mrow></math> </ephtml> decays. Relative uncertainties smaller than 0.05% are indicated by '0.0'. The last bin includes overflows where indicated by the '+' sign</p> <p> <ephtml> <table frame="hsides" rules="groups"><thead><tr><th align="left"><p>Absolute</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi mathvariant="normal">d</mi><mi>σ</mi><mo stretchy="false">/</mo><mi mathvariant="normal">d</mi><mo stretchy="false">(</mo><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>e</mi></msubsup><mo>+</mo><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>μ</mi></msubsup><mo stretchy="false">)</mo></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1830.gif" /></p></th><th align="left"><p>Stat.</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1831.gif" /> mod.</p></th><th align="left"><p>Lept.</p></th><th align="left"><p>Jet/<italic>b</italic></p></th><th align="left"><p>Bkg.</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>L</mi><mo stretchy="false">/</mo><msub><mi>E</mi><mi mathvariant="normal">b</mi></msub></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1832.gif" /></p></th><th align="left"><p>Total</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi mathvariant="normal">d</mi><mi>σ</mi><mo stretchy="false">/</mo><mi mathvariant="normal">d</mi><mo stretchy="false">(</mo><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>e</mi></msubsup><mo>+</mo><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>μ</mi></msubsup><mo stretchy="false">)</mo></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1833.gif" /> (no <math xmlns="http://www.w3.org/1998/Math/MathML"><mi xmlns="">τ</mi></math><inline-graphic href="10052_2020_7907_Article_IEq1834.gif" />)</p></th></tr><tr><th align="left"><p>Bin (<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1835.gif" />)</p></th><th align="left"><p>(fb/<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1836.gif" />)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(fb/<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1837.gif" />)</p></th></tr></thead><tbody><tr><td align="left"><p>40–80</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>96.1</mn><mo>±</mo><mn>2.8</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1838.gif" /></p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.9</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.9</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.9</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>76.1</mn><mo>±</mo><mn>2.2</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1839.gif" /></p></td></tr><tr><td align="left"><p>80–100</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>148.2</mn><mo>±</mo><mn>4.1</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1840.gif" /></p></td><td align="left"><p>0.6</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.8</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>126.3</mn><mo>±</mo><mn>3.4</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1841.gif" /></p></td></tr><tr><td align="left"><p>100–120</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>120.9</mn><mo>±</mo><mn>3.4</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1842.gif" /></p></td><td align="left"><p>0.6</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.7</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>105.9</mn><mo>±</mo><mn>2.9</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1843.gif" /></p></td></tr><tr><td align="left"><p>120–150</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>76.5</mn><mo>±</mo><mn>2.1</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1844.gif" /></p></td><td align="left"><p>0.6</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.8</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>68.1</mn><mo>±</mo><mn>1.8</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1845.gif" /></p></td></tr><tr><td align="left"><p>150–200</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>33.7</mn><mo>±</mo><mn>1.0</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1846.gif" /></p></td><td align="left"><p>0.7</p></td><td align="left"><p>1.1</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.3</p></td><td align="left"><p>1.1</p></td><td align="left"><p>2.4</p></td><td align="left"><p>3.0</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>30.3</mn><mo>±</mo><mn>0.9</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1847.gif" /></p></td></tr><tr><td align="left"><p>200–250</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>11.77</mn><mo>±</mo><mn>0.43</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1848.gif" /></p></td><td align="left"><p>1.3</p></td><td align="left"><p>1.2</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.3</p></td><td align="left"><p>2.0</p></td><td align="left"><p>2.4</p></td><td align="left"><p>3.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>10.65</mn><mo>±</mo><mn>0.38</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1849.gif" /></p></td></tr><tr><td align="left"><p>250–300</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4.57</mn><mo>±</mo><mn>0.23</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1850.gif" /></p></td><td align="left"><p>2.0</p></td><td align="left"><p>1.4</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.3</p></td><td align="left"><p>3.3</p></td><td align="left"><p>2.5</p></td><td align="left"><p>4.9</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4.18</mn><mo>±</mo><mn>0.20</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1851.gif" /></p></td></tr><tr><td align="left"><p>300–400+</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.82</mn><mo>±</mo><mn>0.14</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1852.gif" /></p></td><td align="left"><p>2.4</p></td><td align="left"><p>1.6</p></td><td align="left"><p>1.5</p></td><td align="left"><p>0.6</p></td><td align="left"><p>6.7</p></td><td align="left"><p>2.6</p></td><td align="left"><p>7.9</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.68</mn><mo>±</mo><mn>0.13</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1853.gif" /></p></td></tr></tbody></table> </ephtml> </p> <p>Absolute and normalised differential cross-sections as functions of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>e</mi></msubsup><mo>+</mo><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>μ</mi></msubsup></mrow></math> </ephtml> (top) and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msup><mi>E</mi><mi>e</mi></msup><mo>+</mo><msup><mi>E</mi><mi>μ</mi></msup></mrow></math> </ephtml> (bottom). The columns show the bin ranges, measured cross-section and total uncertainty, relative statistical uncertainty, relative systematic uncertainties in various categories (see text), total relative uncertainty, and differential cross-section corrected to remove contributions via <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>W</mi><mo stretchy="false">→</mo><mi>τ</mi><mo stretchy="false">→</mo><mi>e</mi><mo stretchy="false">/</mo><mi>μ</mi></mrow></math> </ephtml> decays. Relative uncertainties smaller than 0.05% are indicated by '0.0'. The last bin includes overflows where indicated by the '+' sign</p> <p> <ephtml> <table frame="hsides" rules="groups"><thead><tr><th align="left"><p> Normalised</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mfrac><mn>1</mn><mi>σ</mi></mfrac><mi mathvariant="normal">d</mi><mi>σ</mi><mo stretchy="false">/</mo><mi mathvariant="normal">d</mi><mrow><mo stretchy="false">(</mo><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>e</mi></msubsup><mo>+</mo><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>μ</mi></msubsup><mo stretchy="false">)</mo></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1854.gif" /></p></th><th align="left"><p>Stat.</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1855.gif" /> mod.</p></th><th align="left"><p>Lept.</p></th><th align="left"><p>Jet/<italic>b</italic></p></th><th align="left"><p>Bkg.</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>L</mi><mo stretchy="false">/</mo><msub><mi>E</mi><mi mathvariant="normal">b</mi></msub></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1856.gif" /></p></th><th align="left"><p>Total</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mfrac><mn>1</mn><mi>σ</mi></mfrac><mi mathvariant="normal">d</mi><mi>σ</mi><mo stretchy="false">/</mo><mi mathvariant="normal">d</mi><mrow><mo stretchy="false">(</mo><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>e</mi></msubsup><mo>+</mo><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>μ</mi></msubsup><mo stretchy="false">)</mo></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1857.gif" /> (no <math xmlns="http://www.w3.org/1998/Math/MathML"><mi xmlns="">τ</mi></math><inline-graphic href="10052_2020_7907_Article_IEq1858.gif" />)</p></th></tr><tr><th align="left"><p>Bin (<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1859.gif" />)</p></th><th align="left"><p>(<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msup><mn>10</mn><mrow><mo>-</mo><mn>2</mn></mrow></msup><mo stretchy="false">/</mo></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1860.gif" /><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1861.gif" />)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msup><mn>10</mn><mrow><mo>-</mo><mn>2</mn></mrow></msup><mo stretchy="false">/</mo></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1862.gif" /><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1863.gif" />)</p></th></tr></thead><tbody><tr><td align="left"><p>40–80</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.6764</mn><mo>±</mo><mn>0.0066</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1864.gif" /></p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.0</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.6263</mn><mo>±</mo><mn>0.0063</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1865.gif" /></p></td></tr><tr><td align="left"><p>80–100</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.0429</mn><mo>±</mo><mn>0.0079</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1866.gif" /></p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.0393</mn><mo>±</mo><mn>0.0080</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1867.gif" /></p></td></tr><tr><td align="left"><p>100–120</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.8512</mn><mo>±</mo><mn>0.0062</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1868.gif" /></p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.8717</mn><mo>±</mo><mn>0.0064</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1869.gif" /></p></td></tr><tr><td align="left"><p>120–150</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.5387</mn><mo>±</mo><mn>0.0038</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1870.gif" /></p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.5601</mn><mo>±</mo><mn>0.0039</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1871.gif" /></p></td></tr><tr><td align="left"><p>150–200</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.2373</mn><mo>±</mo><mn>0.0027</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1872.gif" /></p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.1</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.2490</mn><mo>±</mo><mn>0.0027</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1873.gif" /></p></td></tr><tr><td align="left"><p>200–250</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.0829</mn><mo>±</mo><mn>0.0020</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1874.gif" /></p></td><td align="left"><p>1.2</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.1</p></td><td align="left"><p>1.8</p></td><td align="left"><p>0.1</p></td><td align="left"><p>2.4</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.0876</mn><mo>±</mo><mn>0.0020</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1875.gif" /></p></td></tr><tr><td align="left"><p>250–300</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.0322</mn><mo>±</mo><mn>0.0013</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1876.gif" /></p></td><td align="left"><p>2.0</p></td><td align="left"><p>1.1</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.3</p></td><td align="left"><p>3.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>4.1</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.0344</mn><mo>±</mo><mn>0.0014</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1877.gif" /></p></td></tr><tr><td align="left"><p>300–400+</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.0128</mn><mo>±</mo><mn>0.0009</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1878.gif" /></p></td><td align="left"><p>2.4</p></td><td align="left"><p>1.5</p></td><td align="left"><p>1.6</p></td><td align="left"><p>0.5</p></td><td align="left"><p>6.6</p></td><td align="left"><p>0.3</p></td><td align="left"><p>7.3</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.0138</mn><mo>±</mo><mn>0.0010</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1879.gif" /></p></td></tr></tbody></table> </ephtml> </p> <p>Absolute and normalised differential cross-sections as functions of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>e</mi></msubsup><mo>+</mo><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>μ</mi></msubsup></mrow></math> </ephtml> (top) and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msup><mi>E</mi><mi>e</mi></msup><mo>+</mo><msup><mi>E</mi><mi>μ</mi></msup></mrow></math> </ephtml> (bottom). The columns show the bin ranges, measured cross-section and total uncertainty, relative statistical uncertainty, relative systematic uncertainties in various categories (see text), total relative uncertainty, and differential cross-section corrected to remove contributions via <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>W</mi><mo stretchy="false">→</mo><mi>τ</mi><mo stretchy="false">→</mo><mi>e</mi><mo stretchy="false">/</mo><mi>μ</mi></mrow></math> </ephtml> decays. Relative uncertainties smaller than 0.05% are indicated by '0.0'. The last bin includes overflows where indicated by the '+' sign</p> <p> <ephtml> <table frame="hsides" rules="groups"><thead><tr><th align="left"><p> Absolute</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi mathvariant="normal">d</mi><mi>σ</mi><mo stretchy="false">/</mo><mi mathvariant="normal">d</mi><mo stretchy="false">(</mo><msup><mi>E</mi><mi>e</mi></msup><mo>+</mo><msup><mi>E</mi><mi>μ</mi></msup><mo stretchy="false">)</mo></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1880.gif" /></p></th><th align="left"><p>Stat.</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1881.gif" /> mod.</p></th><th align="left"><p>Lept.</p></th><th align="left"><p>Jet/<italic>b</italic></p></th><th align="left"><p>Bkg.</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>L</mi><mo stretchy="false">/</mo><msub><mi>E</mi><mi mathvariant="normal">b</mi></msub></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1882.gif" /></p></th><th align="left"><p>Total</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi mathvariant="normal">d</mi><mi>σ</mi><mo stretchy="false">/</mo><mi mathvariant="normal">d</mi><mo stretchy="false">(</mo><msup><mi>E</mi><mi>e</mi></msup><mo>+</mo><msup><mi>E</mi><mi>μ</mi></msup><mo stretchy="false">)</mo></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1883.gif" /> (no <math xmlns="http://www.w3.org/1998/Math/MathML"><mi xmlns="">τ</mi></math><inline-graphic href="10052_2020_7907_Article_IEq1884.gif" />)</p></th></tr><tr><th align="left"><p>Bin (<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1885.gif" />)</p></th><th align="left"><p>(fb/<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1886.gif" />)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(fb/<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1887.gif" />)</p></th></tr></thead><tbody><tr><td align="left"><p>40–80</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>19.82</mn><mo>±</mo><mn>0.63</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1888.gif" /></p></td><td align="left"><p>1.3</p></td><td align="left"><p>0.8</p></td><td align="left"><p>1.2</p></td><td align="left"><p>0.2</p></td><td align="left"><p>1.1</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.2</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>14.95</mn><mo>±</mo><mn>0.47</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1889.gif" /></p></td></tr><tr><td align="left"><p>80–100</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>58.8</mn><mo>±</mo><mn>1.7</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1890.gif" /></p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.9</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.9</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>47.3</mn><mo>±</mo><mn>1.4</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1891.gif" /></p></td></tr><tr><td align="left"><p>100–120</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>71.5</mn><mo>±</mo><mn>2.0</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1892.gif" /></p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.8</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>59.4</mn><mo>±</mo><mn>1.6</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1893.gif" /></p></td></tr><tr><td align="left"><p>120–150</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>71.3</mn><mo>±</mo><mn>2.0</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1894.gif" /></p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.8</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>60.5</mn><mo>±</mo><mn>1.6</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1895.gif" /></p></td></tr><tr><td align="left"><p>150–200</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>57.7</mn><mo>±</mo><mn>1.6</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1896.gif" /></p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.7</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>49.8</mn><mo>±</mo><mn>1.3</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1897.gif" /></p></td></tr><tr><td align="left"><p>200–250</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>39.1</mn><mo>±</mo><mn>1.1</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1898.gif" /></p></td><td align="left"><p>0.7</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.7</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>34.2</mn><mo>±</mo><mn>0.9</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1899.gif" /></p></td></tr><tr><td align="left"><p>250–300</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>25.49</mn><mo>±</mo><mn>0.76</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1900.gif" /></p></td><td align="left"><p>0.9</p></td><td align="left"><p>1.2</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.9</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.0</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>22.57</mn><mo>±</mo><mn>0.65</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1901.gif" /></p></td></tr><tr><td align="left"><p>300–400</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>13.72</mn><mo>±</mo><mn>0.44</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1902.gif" /></p></td><td align="left"><p>0.9</p></td><td align="left"><p>1.3</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.2</p></td><td align="left"><p>1.3</p></td><td align="left"><p>2.4</p></td><td align="left"><p>3.2</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>12.24</mn><mo>±</mo><mn>0.38</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1903.gif" /></p></td></tr><tr><td align="left"><p>400–500</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>5.92</mn><mo>±</mo><mn>0.22</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1904.gif" /></p></td><td align="left"><p>1.4</p></td><td align="left"><p>1.6</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.2</p></td><td align="left"><p>1.9</p></td><td align="left"><p>2.4</p></td><td align="left"><p>3.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>5.33</mn><mo>±</mo><mn>0.19</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1905.gif" /></p></td></tr><tr><td align="left"><p>500–700+</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.66</mn><mo>±</mo><mn>0.13</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1906.gif" /></p></td><td align="left"><p>1.5</p></td><td align="left"><p>1.7</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.3</p></td><td align="left"><p>3.4</p></td><td align="left"><p>2.4</p></td><td align="left"><p>4.9</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.42</mn><mo>±</mo><mn>0.12</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1907.gif" /></p></td></tr></tbody></table> </ephtml> </p> <p>Absolute and normalised differential cross-sections as functions of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>e</mi></msubsup><mo>+</mo><msubsup><mi>p</mi><mrow><mi mathvariant="normal">T</mi></mrow><mi>μ</mi></msubsup></mrow></math> </ephtml> (top) and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msup><mi>E</mi><mi>e</mi></msup><mo>+</mo><msup><mi>E</mi><mi>μ</mi></msup></mrow></math> </ephtml> (bottom). The columns show the bin ranges, measured cross-section and total uncertainty, relative statistical uncertainty, relative systematic uncertainties in various categories (see text), total relative uncertainty, and differential cross-section corrected to remove contributions via <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>W</mi><mo stretchy="false">→</mo><mi>τ</mi><mo stretchy="false">→</mo><mi>e</mi><mo stretchy="false">/</mo><mi>μ</mi></mrow></math> </ephtml> decays. Relative uncertainties smaller than 0.05% are indicated by '0.0'. The last bin includes overflows where indicated by the '+' sign</p> <p> <ephtml> <table frame="hsides" rules="groups"><thead><tr><th align="left"><p> Normalised</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mfrac><mn>1</mn><mi>σ</mi></mfrac><mi mathvariant="normal">d</mi><mi>σ</mi><mo stretchy="false">/</mo><mi mathvariant="normal">d</mi><mrow><mo stretchy="false">(</mo><msup><mi>E</mi><mi>e</mi></msup><mo>+</mo><msup><mi>E</mi><mi>μ</mi></msup><mo stretchy="false">)</mo></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1908.gif" /></p></th><th align="left"><p>Stat.</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1909.gif" /> mod.</p></th><th align="left"><p>Lept.</p></th><th align="left"><p>Jet/<italic>b</italic></p></th><th align="left"><p>Bkg.</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>L</mi><mo stretchy="false">/</mo><msub><mi>E</mi><mi mathvariant="normal">b</mi></msub></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1910.gif" /></p></th><th align="left"><p>Total</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mfrac><mn>1</mn><mi>σ</mi></mfrac><mi mathvariant="normal">d</mi><mi>σ</mi><mo stretchy="false">/</mo><mi mathvariant="normal">d</mi><mrow><mo stretchy="false">(</mo><msup><mi>E</mi><mi>e</mi></msup><mo>+</mo><msup><mi>E</mi><mi>μ</mi></msup><mo stretchy="false">)</mo></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1911.gif" /> (no <math xmlns="http://www.w3.org/1998/Math/MathML"><mi xmlns="">τ</mi></math><inline-graphic href="10052_2020_7907_Article_IEq1912.gif" />)</p></th></tr><tr><th align="left"><p>Bin (<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1913.gif" />)</p></th><th align="left"><p>(<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msup><mn>10</mn><mrow><mo>-</mo><mn>3</mn></mrow></msup><mo stretchy="false">/</mo></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1914.gif" /><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1915.gif" />)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msup><mn>10</mn><mrow><mo>-</mo><mn>3</mn></mrow></msup><mo stretchy="false">/</mo></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1916.gif" /><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1917.gif" />)</p></th></tr></thead><tbody><tr><td align="left"><p>40–80</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.401</mn><mo>±</mo><mn>0.026</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1918.gif" /></p></td><td align="left"><p>1.2</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.1</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.1</p></td><td align="left"><p>1.9</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.234</mn><mo>±</mo><mn>0.023</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1919.gif" /></p></td></tr><tr><td align="left"><p>80–100</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4.157</mn><mo>±</mo><mn>0.056</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1920.gif" /></p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.3</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3.905</mn><mo>±</mo><mn>0.053</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1921.gif" /></p></td></tr><tr><td align="left"><p>100–120</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>5.054</mn><mo>±</mo><mn>0.057</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1922.gif" /></p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.1</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4.900</mn><mo>±</mo><mn>0.056</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1923.gif" /></p></td></tr><tr><td align="left"><p>120–150</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>5.039</mn><mo>±</mo><mn>0.045</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1924.gif" /></p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.9</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4.995</mn><mo>±</mo><mn>0.045</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1925.gif" /></p></td></tr><tr><td align="left"><p>150–200</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4.076</mn><mo>±</mo><mn>0.027</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1926.gif" /></p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4.107</mn><mo>±</mo><mn>0.027</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1927.gif" /></p></td></tr><tr><td align="left"><p>200–250</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.765</mn><mo>±</mo><mn>0.021</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1928.gif" /></p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.0</p></td><td align="left"><p>0.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.826</mn><mo>±</mo><mn>0.022</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1929.gif" /></p></td></tr><tr><td align="left"><p>250–300</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.802</mn><mo>±</mo><mn>0.019</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1930.gif" /></p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.1</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.863</mn><mo>±</mo><mn>0.020</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1931.gif" /></p></td></tr><tr><td align="left"><p>300–400</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.970</mn><mo>±</mo><mn>0.014</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1932.gif" /></p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.4</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.010</mn><mo>±</mo><mn>0.014</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1933.gif" /></p></td></tr><tr><td align="left"><p>400–500</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.4187</mn><mo>±</mo><mn>0.0097</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1934.gif" /></p></td><td align="left"><p>1.3</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.1</p></td><td align="left"><p>1.5</p></td><td align="left"><p>0.1</p></td><td align="left"><p>2.3</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.4397</mn><mo>±</mo><mn>0.0099</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1935.gif" /></p></td></tr><tr><td align="left"><p>500–700+</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.1879</mn><mo>±</mo><mn>0.0070</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1936.gif" /></p></td><td align="left"><p>1.5</p></td><td align="left"><p>1.2</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.1</p></td><td align="left"><p>3.1</p></td><td align="left"><p>0.1</p></td><td align="left"><p>3.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.1998</mn><mo>±</mo><mn>0.0074</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1937.gif" /></p></td></tr></tbody></table> </ephtml> </p> <p>Absolute differential cross-sections as a function of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>η</mi><mi>ℓ</mi></msup><mrow><mo stretchy="false">|</mo><mo>×</mo></mrow><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math> </ephtml> . The columns show the bin ranges, measured cross-section and total uncertainty, relative statistical uncertainty, relative systematic uncertainties in various categories (see text), total relative uncertainty, and differential cross-section corrected to remove contributions via <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>W</mi><mo stretchy="false">→</mo><mi>τ</mi><mo stretchy="false">→</mo><mi>e</mi><mo stretchy="false">/</mo><mi>μ</mi></mrow></math> </ephtml> decays. Relative uncertainties smaller than 0.05% are indicated by '0.0'. The last bin includes overflows where indicated by the '+' sign</p> <p> <ephtml> <table frame="hsides" rules="groups"><thead><tr><th align="left"><p>Absolute</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msup><mi mathvariant="normal">d</mi><mn>2</mn></msup><mi>σ</mi><mo stretchy="false">/</mo><mi mathvariant="normal">d</mi><mrow><mo stretchy="false">|</mo><msup><mi>η</mi><mi>ℓ</mi></msup><mo stretchy="false">|</mo></mrow><mi mathvariant="normal">d</mi><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1940.gif" /></p></th><th align="left"><p>Stat.</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1941.gif" /> mod.</p></th><th align="left"><p>Lept.</p></th><th align="left"><p>Jet/<italic>b</italic></p></th><th align="left"><p>Bkg.</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>L</mi><mo stretchy="false">/</mo><msub><mi>E</mi><mi mathvariant="normal">b</mi></msub></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1942.gif" /></p></th><th align="left"><p>Total</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msup><mi mathvariant="normal">d</mi><mn>2</mn></msup><mi>σ</mi><mo stretchy="false">/</mo><mi mathvariant="normal">d</mi><mrow><mo stretchy="false">|</mo><msup><mi>η</mi><mi>ℓ</mi></msup><mo stretchy="false">|</mo></mrow><mi mathvariant="normal">d</mi><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1943.gif" /></p></th></tr><tr><th align="left" /><th align="left" /><th align="left" /><th align="left" /><th align="left" /><th align="left" /><th align="left" /><th align="left" /><th align="left" /><th align="left"><p>(no <math xmlns="http://www.w3.org/1998/Math/MathML"><mi xmlns="">τ</mi></math><inline-graphic href="10052_2020_7907_Article_IEq1944.gif" />)</p></th></tr><tr><th align="left"><p>Bin (unit <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mo stretchy="false">|</mo><mi>η</mi><mo stretchy="false">|</mo></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1945.gif" /><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1946.gif" />)</p></th><th align="left"><p>(fb/unit <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mo stretchy="false">|</mo><mi>η</mi><mo stretchy="false">|</mo></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1947.gif" /><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1948.gif" />)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(fb/unit <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mo stretchy="false">|</mo><mi>η</mi><mo stretchy="false">|</mo></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1949.gif" /><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1950.gif" />)</p></th></tr></thead><tbody><tr><td align="left" colspan="10"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0</mn><mo><</mo><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mo><</mo><mn>80</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1951.gif" /></p></td></tr><tr><td align="left"><p>   0.00–0.25</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>87.2</mn><mo>±</mo><mn>2.5</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1952.gif" /></p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.1</p></td><td align="left"><p>1.0</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>72.3</mn><mo>±</mo><mn>2.0</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1953.gif" /></p></td></tr><tr><td align="left"><p>   0.25–0.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>82.6</mn><mo>±</mo><mn>2.3</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1954.gif" /></p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.9</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>68.5</mn><mo>±</mo><mn>1.9</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1955.gif" /></p></td></tr><tr><td align="left"><p>   0.50–0.75</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>78.2</mn><mo>±</mo><mn>2.2</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1956.gif" /></p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.8</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.9</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>65.0</mn><mo>±</mo><mn>1.8</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1957.gif" /></p></td></tr><tr><td align="left"><p>   0.75–1.00</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>70.2</mn><mo>±</mo><mn>2.1</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1958.gif" /></p></td><td align="left"><p>0.9</p></td><td align="left"><p>1.1</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.9</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.0</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>58.3</mn><mo>±</mo><mn>1.7</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1959.gif" /></p></td></tr><tr><td align="left"><p>   1.00–1.25</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>60.0</mn><mo>±</mo><mn>1.9</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1960.gif" /></p></td><td align="left"><p>0.9</p></td><td align="left"><p>1.3</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.9</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.1</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>50.0</mn><mo>±</mo><mn>1.5</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1961.gif" /></p></td></tr><tr><td align="left"><p>   1.25–1.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>51.5</mn><mo>±</mo><mn>1.7</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1962.gif" /></p></td><td align="left"><p>1.2</p></td><td align="left"><p>1.5</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.1</p></td><td align="left"><p>1.0</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.3</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>42.9</mn><mo>±</mo><mn>1.3</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1963.gif" /></p></td></tr><tr><td align="left"><p>   1.50–1.75</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>41.0</mn><mo>±</mo><mn>1.4</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1964.gif" /></p></td><td align="left"><p>1.3</p></td><td align="left"><p>1.7</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.2</p></td><td align="left"><p>1.0</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.4</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>34.2</mn><mo>±</mo><mn>1.1</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1965.gif" /></p></td></tr><tr><td align="left"><p>   1.75–2.00</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>31.4</mn><mo>±</mo><mn>1.2</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1966.gif" /></p></td><td align="left"><p>1.5</p></td><td align="left"><p>1.8</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.2</p></td><td align="left"><p>1.2</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>26.2</mn><mo>±</mo><mn>0.9</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1967.gif" /></p></td></tr><tr><td align="left"><p>   2.00–2.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>18.45</mn><mo>±</mo><mn>0.73</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1968.gif" /></p></td><td align="left"><p>1.5</p></td><td align="left"><p>2.2</p></td><td align="left"><p>1.1</p></td><td align="left"><p>0.3</p></td><td align="left"><p>1.5</p></td><td align="left"><p>2.3</p></td><td align="left"><p>4.0</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>15.42</mn><mo>±</mo><mn>0.57</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1969.gif" /></p></td></tr><tr><td align="left" colspan="10"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>80</mn><mo><</mo><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mo><</mo><mn>120</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1970.gif" /></p></td></tr><tr><td align="left"><p>   0.00–0.25</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>120.6</mn><mo>±</mo><mn>3.4</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1971.gif" /></p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.8</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.9</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>102.2</mn><mo>±</mo><mn>3.0</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1972.gif" /></p></td></tr><tr><td align="left"><p>   0.25–0.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>113.5</mn><mo>±</mo><mn>3.2</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1973.gif" /></p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.7</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>96.3</mn><mo>±</mo><mn>2.7</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1974.gif" /></p></td></tr><tr><td align="left"><p>   0.50–0.75</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>105.5</mn><mo>±</mo><mn>3.0</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1975.gif" /></p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.7</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>89.5</mn><mo>±</mo><mn>2.5</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1976.gif" /></p></td></tr><tr><td align="left"><p>   0.75–1.00</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>93.2</mn><mo>±</mo><mn>2.7</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1977.gif" /></p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.7</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.9</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>79.1</mn><mo>±</mo><mn>2.3</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1978.gif" /></p></td></tr><tr><td align="left"><p>   1.00–1.25</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>82.3</mn><mo>±</mo><mn>2.4</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1979.gif" /></p></td><td align="left"><p>1.1</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.7</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.9</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>69.9</mn><mo>±</mo><mn>2.0</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1980.gif" /></p></td></tr><tr><td align="left"><p>   1.25–1.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>69.5</mn><mo>±</mo><mn>2.1</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1981.gif" /></p></td><td align="left"><p>1.3</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.8</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.0</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>58.9</mn><mo>±</mo><mn>1.8</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1982.gif" /></p></td></tr><tr><td align="left"><p>   1.50–1.75</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>57.1</mn><mo>±</mo><mn>1.8</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1983.gif" /></p></td><td align="left"><p>1.4</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.9</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.1</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>48.4</mn><mo>±</mo><mn>1.5</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1984.gif" /></p></td></tr><tr><td align="left"><p>   1.75–2.00</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>45.0</mn><mo>±</mo><mn>1.5</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1985.gif" /></p></td><td align="left"><p>1.6</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.3</p></td><td align="left"><p>1.0</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.2</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>38.4</mn><mo>±</mo><mn>1.2</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1986.gif" /></p></td></tr><tr><td align="left"><p>   2.00–2.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>28.85</mn><mo>±</mo><mn>0.97</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1987.gif" /></p></td><td align="left"><p>1.5</p></td><td align="left"><p>1.1</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.3</p></td><td align="left"><p>1.3</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.4</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>24.53</mn><mo>±</mo><mn>0.83</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1988.gif" /></p></td></tr><tr><td align="left" colspan="10"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>120</mn><mo><</mo><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mo><</mo><mn>200</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1989.gif" /></p></td></tr><tr><td align="left"><p>   0.00–0.25</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>50.6</mn><mo>±</mo><mn>1.6</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1990.gif" /></p></td><td align="left"><p>0.9</p></td><td align="left"><p>1.7</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.8</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.2</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>44.5</mn><mo>±</mo><mn>1.3</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1991.gif" /></p></td></tr><tr><td align="left"><p>   0.25–0.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>48.4</mn><mo>±</mo><mn>1.5</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1992.gif" /></p></td><td align="left"><p>0.9</p></td><td align="left"><p>1.6</p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.8</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.1</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>42.5</mn><mo>±</mo><mn>1.3</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1993.gif" /></p></td></tr><tr><td align="left"><p>   0.50–0.75</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>46.7</mn><mo>±</mo><mn>1.4</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1994.gif" /></p></td><td align="left"><p>0.9</p></td><td align="left"><p>1.5</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.7</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.1</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>40.9</mn><mo>±</mo><mn>1.2</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1995.gif" /></p></td></tr><tr><td align="left"><p>   0.75–1.00</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>44.0</mn><mo>±</mo><mn>1.3</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1996.gif" /></p></td><td align="left"><p>1.0</p></td><td align="left"><p>1.4</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.7</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.0</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>38.6</mn><mo>±</mo><mn>1.1</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1997.gif" /></p></td></tr><tr><td align="left"><p>   1.00–1.25</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>38.9</mn><mo>±</mo><mn>1.2</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1998.gif" /></p></td><td align="left"><p>1.1</p></td><td align="left"><p>1.3</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.8</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.1</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>34.1</mn><mo>±</mo><mn>1.0</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq1999.gif" /></p></td></tr><tr><td align="left"><p>   1.25–1.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>34.3</mn><mo>±</mo><mn>1.1</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2000.gif" /></p></td><td align="left"><p>1.3</p></td><td align="left"><p>1.3</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.8</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.2</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>30.0</mn><mo>±</mo><mn>0.9</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2001.gif" /></p></td></tr><tr><td align="left"><p>   1.50–1.75</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>28.79</mn><mo>±</mo><mn>0.92</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2002.gif" /></p></td><td align="left"><p>1.3</p></td><td align="left"><p>1.3</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.3</p></td><td align="left"><p>1.0</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.2</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>25.20</mn><mo>±</mo><mn>0.79</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2003.gif" /></p></td></tr><tr><td align="left"><p>   1.75–2.00</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>23.97</mn><mo>±</mo><mn>0.78</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2004.gif" /></p></td><td align="left"><p>1.4</p></td><td align="left"><p>1.3</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.2</p></td><td align="left"><p>1.0</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.2</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>20.98</mn><mo>±</mo><mn>0.67</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2005.gif" /></p></td></tr><tr><td align="left"><p>   2.00–2.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>16.46</mn><mo>±</mo><mn>0.54</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2006.gif" /></p></td><td align="left"><p>1.3</p></td><td align="left"><p>1.2</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.2</p></td><td align="left"><p>1.3</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.3</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>14.43</mn><mo>±</mo><mn>0.47</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2007.gif" /></p></td></tr><tr><td align="left" colspan="10"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>200</mn><mo><</mo><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mo><</mo><mn>500</mn><mo>+</mo><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2008.gif" /></p></td></tr><tr><td align="left"><p>   0.00–0.25</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4.90</mn><mo>±</mo><mn>0.18</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2009.gif" /></p></td><td align="left"><p>1.6</p></td><td align="left"><p>1.3</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.3</p></td><td align="left"><p>1.8</p></td><td align="left"><p>2.4</p></td><td align="left"><p>3.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4.47</mn><mo>±</mo><mn>0.17</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2010.gif" /></p></td></tr><tr><td align="left"><p>   0.25–0.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>5.09</mn><mo>±</mo><mn>0.19</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2011.gif" /></p></td><td align="left"><p>1.5</p></td><td align="left"><p>1.2</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.3</p></td><td align="left"><p>1.9</p></td><td align="left"><p>2.4</p></td><td align="left"><p>3.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4.65</mn><mo>±</mo><mn>0.17</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2012.gif" /></p></td></tr><tr><td align="left"><p>   0.50–0.75</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4.95</mn><mo>±</mo><mn>0.18</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2013.gif" /></p></td><td align="left"><p>1.5</p></td><td align="left"><p>1.2</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.3</p></td><td align="left"><p>2.0</p></td><td align="left"><p>2.4</p></td><td align="left"><p>3.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4.52</mn><mo>±</mo><mn>0.17</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2014.gif" /></p></td></tr><tr><td align="left"><p>   0.75–1.00</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4.93</mn><mo>±</mo><mn>0.18</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2015.gif" /></p></td><td align="left"><p>1.5</p></td><td align="left"><p>1.2</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.4</p></td><td align="left"><p>1.9</p></td><td align="left"><p>2.4</p></td><td align="left"><p>3.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4.50</mn><mo>±</mo><mn>0.16</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2016.gif" /></p></td></tr><tr><td align="left"><p>   1.00–1.25</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4.91</mn><mo>±</mo><mn>0.18</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2017.gif" /></p></td><td align="left"><p>1.5</p></td><td align="left"><p>1.3</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.2</p></td><td align="left"><p>1.9</p></td><td align="left"><p>2.4</p></td><td align="left"><p>3.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4.46</mn><mo>±</mo><mn>0.16</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2018.gif" /></p></td></tr><tr><td align="left"><p>   1.25–1.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4.42</mn><mo>±</mo><mn>0.18</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2019.gif" /></p></td><td align="left"><p>1.9</p></td><td align="left"><p>1.5</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.6</p></td><td align="left"><p>2.0</p></td><td align="left"><p>2.4</p></td><td align="left"><p>4.0</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4.01</mn><mo>±</mo><mn>0.16</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2020.gif" /></p></td></tr><tr><td align="left"><p>   1.50–1.75</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4.18</mn><mo>±</mo><mn>0.16</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2021.gif" /></p></td><td align="left"><p>1.7</p></td><td align="left"><p>1.5</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.3</p></td><td align="left"><p>1.8</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.9</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3.80</mn><mo>±</mo><mn>0.14</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2022.gif" /></p></td></tr><tr><td align="left"><p>   1.75–2.00</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3.70</mn><mo>±</mo><mn>0.15</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2023.gif" /></p></td><td align="left"><p>1.9</p></td><td align="left"><p>1.8</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.3</p></td><td align="left"><p>1.9</p></td><td align="left"><p>2.3</p></td><td align="left"><p>4.0</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3.36</mn><mo>±</mo><mn>0.13</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2024.gif" /></p></td></tr><tr><td align="left"><p>   2.00–2.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.71</mn><mo>±</mo><mn>0.11</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2025.gif" /></p></td><td align="left"><p>1.6</p></td><td align="left"><p>2.0</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.3</p></td><td align="left"><p>1.9</p></td><td align="left"><p>2.3</p></td><td align="left"><p>4.0</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.46</mn><mo>±</mo><mn>0.10</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2026.gif" /></p></td></tr></tbody></table> </ephtml> </p> <p>Normalised differential cross-sections as a function of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>η</mi><mi>ℓ</mi></msup><mrow><mo stretchy="false">|</mo><mo>×</mo></mrow><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math> </ephtml> . The columns show the bin ranges, measured cross-section and total uncertainty, relative statistical uncertainty, relative systematic uncertainties in various categories (see text), total relative uncertainty, and differential cross-section corrected to remove contributions via <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>W</mi><mo stretchy="false">→</mo><mi>τ</mi><mo stretchy="false">→</mo><mi>e</mi><mo stretchy="false">/</mo><mi>μ</mi></mrow></math> </ephtml> decays. Relative uncertainties smaller than 0.05% are indicated by '0.0'. The last bin includes overflows where indicated by the '+' sign</p> <p> <ephtml> <table frame="hsides" rules="groups"><thead><tr><th align="left"><p>Normalised</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mfrac><mn>1</mn><mi>σ</mi></mfrac><msup><mi mathvariant="normal">d</mi><mn>2</mn></msup><mi>σ</mi><mo stretchy="false">/</mo><mi mathvariant="normal">d</mi><mrow><mo stretchy="false">|</mo><msup><mi>η</mi><mi>ℓ</mi></msup><mo stretchy="false">|</mo></mrow><mi mathvariant="normal">d</mi><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2029.gif" /></p></th><th align="left"><p>Stat.</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2030.gif" /> mod.</p></th><th align="left"><p>Lept.</p></th><th align="left"><p>Jet/<italic>b</italic></p></th><th align="left"><p>Bkg.</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>L</mi><mo stretchy="false">/</mo><msub><mi>E</mi><mi mathvariant="normal">b</mi></msub></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2031.gif" /></p></th><th align="left"><p>Total</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mfrac><mn>1</mn><mi>σ</mi></mfrac><msup><mi mathvariant="normal">d</mi><mn>2</mn></msup><mi>σ</mi><mo stretchy="false">/</mo><mi mathvariant="normal">d</mi><mrow><mo stretchy="false">|</mo><msup><mi>η</mi><mi>ℓ</mi></msup><mo stretchy="false">|</mo></mrow><mi mathvariant="normal">d</mi><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2032.gif" /></p></th></tr><tr><th align="left" /><th align="left" /><th align="left" /><th align="left" /><th align="left" /><th align="left" /><th align="left" /><th align="left" /><th align="left" /><th align="left"><p>(no <math xmlns="http://www.w3.org/1998/Math/MathML"><mi xmlns="">τ</mi></math><inline-graphic href="10052_2020_7907_Article_IEq2033.gif" />)</p></th></tr><tr><th align="left"><p>Bin (unit <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mo stretchy="false">|</mo><mi>η</mi><mo stretchy="false">|</mo></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2034.gif" /><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2035.gif" />)</p></th><th align="left"><p>(<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msup><mn>10</mn><mrow><mo>-</mo><mn>3</mn></mrow></msup><mo stretchy="false">/</mo></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2036.gif" />unit <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mo stretchy="false">|</mo><mi>η</mi><mo stretchy="false">|</mo></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2037.gif" /><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2038.gif" />)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msup><mn>10</mn><mrow><mo>-</mo><mn>3</mn></mrow></msup><mo stretchy="false">/</mo></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2039.gif" />unit <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mo stretchy="false">|</mo><mi>η</mi><mo stretchy="false">|</mo></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2040.gif" /><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2041.gif" />)</p></th></tr></thead><tbody><tr><td align="left" colspan="10"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0</mn><mo><</mo><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mo><</mo><mn>80</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2042.gif" /></p></td></tr><tr><td align="left"><p>   0.00–0.25</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3.072</mn><mo>±</mo><mn>0.042</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2043.gif" /></p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.4</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.977</mn><mo>±</mo><mn>0.039</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2044.gif" /></p></td></tr><tr><td align="left"><p>   0.25–0.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.909</mn><mo>±</mo><mn>0.037</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2045.gif" /></p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.3</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.819</mn><mo>±</mo><mn>0.034</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2046.gif" /></p></td></tr><tr><td align="left"><p>   0.50–0.75</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.757</mn><mo>±</mo><mn>0.034</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2047.gif" /></p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.2</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.675</mn><mo>±</mo><mn>0.031</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2048.gif" /></p></td></tr><tr><td align="left"><p>   0.75–1.00</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.473</mn><mo>±</mo><mn>0.032</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2049.gif" /></p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.3</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.398</mn><mo>±</mo><mn>0.030</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2050.gif" /></p></td></tr><tr><td align="left"><p>   1.00–1.25</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.115</mn><mo>±</mo><mn>0.030</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2051.gif" /></p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.4</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.057</mn><mo>±</mo><mn>0.028</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2052.gif" /></p></td></tr><tr><td align="left"><p>   1.25–1.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.815</mn><mo>±</mo><mn>0.031</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2053.gif" /></p></td><td align="left"><p>1.2</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.765</mn><mo>±</mo><mn>0.029</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2054.gif" /></p></td></tr><tr><td align="left"><p>   1.50–1.75</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.444</mn><mo>±</mo><mn>0.028</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2055.gif" /></p></td><td align="left"><p>1.2</p></td><td align="left"><p>1.2</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.9</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.406</mn><mo>±</mo><mn>0.025</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2056.gif" /></p></td></tr><tr><td align="left"><p>   1.75–2.00</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.106</mn><mo>±</mo><mn>0.025</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2057.gif" /></p></td><td align="left"><p>1.5</p></td><td align="left"><p>1.4</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.0</p></td><td align="left"><p>2.2</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.079</mn><mo>±</mo><mn>0.023</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2058.gif" /></p></td></tr><tr><td align="left"><p>   2.00–2.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.650</mn><mo>±</mo><mn>0.016</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2059.gif" /></p></td><td align="left"><p>1.4</p></td><td align="left"><p>1.6</p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.2</p></td><td align="left"><p>1.2</p></td><td align="left"><p>0.0</p></td><td align="left"><p>2.5</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.635</mn><mo>±</mo><mn>0.015</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2060.gif" /></p></td></tr><tr><td align="left" colspan="10"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>80</mn><mo><</mo><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mo><</mo><mn>120</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2061.gif" /></p></td></tr><tr><td align="left"><p>   0.00–0.25</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4.248</mn><mo>±</mo><mn>0.051</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2062.gif" /></p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.2</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4.208</mn><mo>±</mo><mn>0.054</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2063.gif" /></p></td></tr><tr><td align="left"><p>   0.25–0.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3.999</mn><mo>±</mo><mn>0.045</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2064.gif" /></p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.1</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3.963</mn><mo>±</mo><mn>0.046</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2065.gif" /></p></td></tr><tr><td align="left"><p>   0.50–0.75</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3.716</mn><mo>±</mo><mn>0.043</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2066.gif" /></p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.1</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3.685</mn><mo>±</mo><mn>0.042</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2067.gif" /></p></td></tr><tr><td align="left"><p>   0.75–1.00</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3.283</mn><mo>±</mo><mn>0.040</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2068.gif" /></p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.2</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3.255</mn><mo>±</mo><mn>0.039</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2069.gif" /></p></td></tr><tr><td align="left"><p>   1.00–1.25</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.900</mn><mo>±</mo><mn>0.036</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2070.gif" /></p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.3</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.878</mn><mo>±</mo><mn>0.036</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2071.gif" /></p></td></tr><tr><td align="left"><p>   1.25–1.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.448</mn><mo>±</mo><mn>0.038</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2072.gif" /></p></td><td align="left"><p>1.3</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.6</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.425</mn><mo>±</mo><mn>0.038</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2073.gif" /></p></td></tr><tr><td align="left"><p>   1.50–1.75</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.011</mn><mo>±</mo><mn>0.032</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2074.gif" /></p></td><td align="left"><p>1.4</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.6</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.992</mn><mo>±</mo><mn>0.032</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2075.gif" /></p></td></tr><tr><td align="left"><p>   1.75–2.00</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.586</mn><mo>±</mo><mn>0.029</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2076.gif" /></p></td><td align="left"><p>1.5</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.9</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.581</mn><mo>±</mo><mn>0.030</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2077.gif" /></p></td></tr><tr><td align="left"><p>   2.00–2.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.017</mn><mo>±</mo><mn>0.019</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2078.gif" /></p></td><td align="left"><p>1.4</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.9</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.010</mn><mo>±</mo><mn>0.019</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2079.gif" /></p></td></tr><tr><td align="left" colspan="10"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>120</mn><mo><</mo><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mo><</mo><mn>200</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2080.gif" /></p></td></tr><tr><td align="left"><p>   0.00–0.25</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.783</mn><mo>±</mo><mn>0.028</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2081.gif" /></p></td><td align="left"><p>0.9</p></td><td align="left"><p>1.2</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.6</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.832</mn><mo>±</mo><mn>0.025</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2082.gif" /></p></td></tr><tr><td align="left"><p>   0.25–0.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.706</mn><mo>±</mo><mn>0.025</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2083.gif" /></p></td><td align="left"><p>0.9</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.5</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.751</mn><mo>±</mo><mn>0.023</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2084.gif" /></p></td></tr><tr><td align="left"><p>   0.50–0.75</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.645</mn><mo>±</mo><mn>0.022</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2085.gif" /></p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.4</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.685</mn><mo>±</mo><mn>0.022</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2086.gif" /></p></td></tr><tr><td align="left"><p>   0.75–1.00</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.549</mn><mo>±</mo><mn>0.021</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2087.gif" /></p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.3</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.587</mn><mo>±</mo><mn>0.021</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2088.gif" /></p></td></tr><tr><td align="left"><p>   1.00–1.25</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.370</mn><mo>±</mo><mn>0.018</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2089.gif" /></p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.3</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.402</mn><mo>±</mo><mn>0.019</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2090.gif" /></p></td></tr><tr><td align="left"><p>   1.25–1.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.208</mn><mo>±</mo><mn>0.019</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2091.gif" /></p></td><td align="left"><p>1.3</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.6</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.235</mn><mo>±</mo><mn>0.019</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2092.gif" /></p></td></tr><tr><td align="left"><p>   1.50–1.75</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.014</mn><mo>±</mo><mn>0.016</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2093.gif" /></p></td><td align="left"><p>1.3</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.6</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.037</mn><mo>±</mo><mn>0.016</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2094.gif" /></p></td></tr><tr><td align="left"><p>   1.75–2.00</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.845</mn><mo>±</mo><mn>0.015</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2095.gif" /></p></td><td align="left"><p>1.4</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.863</mn><mo>±</mo><mn>0.015</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2096.gif" /></p></td></tr><tr><td align="left"><p>   2.00–2.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.5801</mn><mo>±</mo><mn>0.0098</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2097.gif" /></p></td><td align="left"><p>1.3</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.5938</mn><mo>±</mo><mn>0.0100</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2098.gif" /></p></td></tr><tr><td align="left" colspan="10"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>200</mn><mo><</mo><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mo><</mo><mn>500</mn><mo>+</mo><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2099.gif" /></p></td></tr><tr><td align="left"><p>   0.00–0.25</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.1728</mn><mo>±</mo><mn>0.0047</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2100.gif" /></p></td><td align="left"><p>1.6</p></td><td align="left"><p>1.5</p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.2</p></td><td align="left"><p>1.6</p></td><td align="left"><p>0.1</p></td><td align="left"><p>2.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.1840</mn><mo>±</mo><mn>0.0050</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2101.gif" /></p></td></tr><tr><td align="left"><p>   0.25–0.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.1793</mn><mo>±</mo><mn>0.0047</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2102.gif" /></p></td><td align="left"><p>1.5</p></td><td align="left"><p>1.3</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.2</p></td><td align="left"><p>1.7</p></td><td align="left"><p>0.1</p></td><td align="left"><p>2.6</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.1914</mn><mo>±</mo><mn>0.0050</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2103.gif" /></p></td></tr><tr><td align="left"><p>   0.50–0.75</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.1744</mn><mo>±</mo><mn>0.0046</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2104.gif" /></p></td><td align="left"><p>1.5</p></td><td align="left"><p>1.1</p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.1</p></td><td align="left"><p>1.8</p></td><td align="left"><p>0.1</p></td><td align="left"><p>2.6</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.1859</mn><mo>±</mo><mn>0.0048</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2105.gif" /></p></td></tr><tr><td align="left"><p>   0.75–1.00</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.1736</mn><mo>±</mo><mn>0.0044</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2106.gif" /></p></td><td align="left"><p>1.5</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.2</p></td><td align="left"><p>1.7</p></td><td align="left"><p>0.0</p></td><td align="left"><p>2.6</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.1853</mn><mo>±</mo><mn>0.0047</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2107.gif" /></p></td></tr><tr><td align="left"><p>   1.00–1.25</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.1729</mn><mo>±</mo><mn>0.0043</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2108.gif" /></p></td><td align="left"><p>1.5</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.2</p></td><td align="left"><p>1.7</p></td><td align="left"><p>0.0</p></td><td align="left"><p>2.5</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.1837</mn><mo>±</mo><mn>0.0046</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2109.gif" /></p></td></tr><tr><td align="left"><p>   1.25–1.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.1559</mn><mo>±</mo><mn>0.0045</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2110.gif" /></p></td><td align="left"><p>1.9</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.6</p></td><td align="left"><p>1.8</p></td><td align="left"><p>0.0</p></td><td align="left"><p>2.9</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.1652</mn><mo>±</mo><mn>0.0048</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2111.gif" /></p></td></tr><tr><td align="left"><p>   1.50–1.75</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.1474</mn><mo>±</mo><mn>0.0039</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2112.gif" /></p></td><td align="left"><p>1.7</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.2</p></td><td align="left"><p>1.6</p></td><td align="left"><p>0.0</p></td><td align="left"><p>2.6</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.1563</mn><mo>±</mo><mn>0.0041</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2113.gif" /></p></td></tr><tr><td align="left"><p>   1.75–2.00</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.1303</mn><mo>±</mo><mn>0.0037</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2114.gif" /></p></td><td align="left"><p>1.9</p></td><td align="left"><p>1.1</p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.2</p></td><td align="left"><p>1.6</p></td><td align="left"><p>0.0</p></td><td align="left"><p>2.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.1382</mn><mo>±</mo><mn>0.0039</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2115.gif" /></p></td></tr><tr><td align="left"><p>   2.00–2.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.0955</mn><mo>±</mo><mn>0.0026</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2116.gif" /></p></td><td align="left"><p>1.6</p></td><td align="left"><p>1.3</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.3</p></td><td align="left"><p>1.7</p></td><td align="left"><p>0.1</p></td><td align="left"><p>2.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.1012</mn><mo>±</mo><mn>0.0027</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2117.gif" /></p></td></tr></tbody></table> </ephtml> </p> <p>Absolute differential cross-sections as a function of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>y</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mrow><mo stretchy="false">|</mo><mo>×</mo></mrow><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math> </ephtml> . The columns show the bin ranges, measured cross-section and total uncertainty, relative statistical uncertainty, relative systematic uncertainties in various categories (see text), total relative uncertainty, and differential cross-section corrected to remove contributions via <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>W</mi><mo stretchy="false">→</mo><mi>τ</mi><mo stretchy="false">→</mo><mi>e</mi><mo stretchy="false">/</mo><mi>μ</mi></mrow></math> </ephtml> decays. Relative uncertainties smaller than 0.05% are indicated by '0.0'. The last bin includes overflows where indicated by the '+' sign</p> <p> <ephtml> <table frame="hsides" rules="groups"><thead><tr><th align="left"><p>Absolute</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msup><mi mathvariant="normal">d</mi><mn>2</mn></msup><mi>σ</mi><mo stretchy="false">/</mo><mi mathvariant="normal">d</mi><mrow><mo stretchy="false">|</mo><msup><mi>y</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mo stretchy="false">|</mo></mrow><mi mathvariant="normal">d</mi><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2120.gif" /></p></th><th align="left"><p>Stat.</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2121.gif" /> mod.</p></th><th align="left"><p>Lept.</p></th><th align="left"><p>Jet/<italic>b</italic></p></th><th align="left"><p>Bkg.</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>L</mi><mo stretchy="false">/</mo><msub><mi>E</mi><mi mathvariant="normal">b</mi></msub></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2122.gif" /></p></th><th align="left"><p>Total</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msup><mi mathvariant="normal">d</mi><mn>2</mn></msup><mi>σ</mi><mo stretchy="false">/</mo><mi mathvariant="normal">d</mi><mrow><mo stretchy="false">|</mo><msup><mi>y</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mo stretchy="false">|</mo></mrow><mi mathvariant="normal">d</mi><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2123.gif" /></p></th></tr><tr><th align="left" /><th align="left" /><th align="left" /><th align="left" /><th align="left" /><th align="left" /><th align="left" /><th align="left" /><th align="left" /><th align="left"><p>(no <math xmlns="http://www.w3.org/1998/Math/MathML"><mi xmlns="">τ</mi></math><inline-graphic href="10052_2020_7907_Article_IEq2124.gif" />)</p></th></tr><tr><th align="left"><p>Bin (unit |<italic>y</italic>| <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2125.gif" />)</p></th><th align="left"><p>(fb/unit |<italic>y</italic>| <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2126.gif" />)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(fb/unit |<italic>y</italic>| <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2127.gif" />)</p></th></tr></thead><tbody><tr><td align="left" colspan="10"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0</mn><mo><</mo><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mo><</mo><mn>80</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2128.gif" /></p></td></tr><tr><td align="left"><p>   0.00–0.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>44.9</mn><mo>±</mo><mn>1.3</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2129.gif" /></p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.9</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>37.1</mn><mo>±</mo><mn>1.0</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2130.gif" /></p></td></tr><tr><td align="left"><p>   0.50–1.00</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>38.7</mn><mo>±</mo><mn>1.1</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2131.gif" /></p></td><td align="left"><p>0.8</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.9</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.9</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>32.1</mn><mo>±</mo><mn>0.9</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2132.gif" /></p></td></tr><tr><td align="left"><p>   1.00–1.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>29.48</mn><mo>±</mo><mn>0.95</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2133.gif" /></p></td><td align="left"><p>1.0</p></td><td align="left"><p>1.4</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.2</p></td><td align="left"><p>1.0</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.2</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>24.56</mn><mo>±</mo><mn>0.74</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2134.gif" /></p></td></tr><tr><td align="left"><p>   1.50–2.00</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>17.38</mn><mo>±</mo><mn>0.65</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2135.gif" /></p></td><td align="left"><p>1.5</p></td><td align="left"><p>1.9</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.4</p></td><td align="left"><p>1.3</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>14.58</mn><mo>±</mo><mn>0.52</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2136.gif" /></p></td></tr><tr><td align="left"><p>   2.00–2.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4.13</mn><mo>±</mo><mn>0.24</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2137.gif" /></p></td><td align="left"><p>3.4</p></td><td align="left"><p>2.9</p></td><td align="left"><p>1.2</p></td><td align="left"><p>0.5</p></td><td align="left"><p>2.5</p></td><td align="left"><p>2.4</p></td><td align="left"><p>5.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3.49</mn><mo>±</mo><mn>0.20</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2138.gif" /></p></td></tr><tr><td align="left" colspan="10"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>80</mn><mo><</mo><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mo><</mo><mn>120</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2139.gif" /></p></td></tr><tr><td align="left"><p>   0.00–0.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>67.4</mn><mo>±</mo><mn>1.9</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2140.gif" /></p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.8</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>57.0</mn><mo>±</mo><mn>1.6</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2141.gif" /></p></td></tr><tr><td align="left"><p>   0.50–1.00</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>56.9</mn><mo>±</mo><mn>1.6</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2142.gif" /></p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.7</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>48.2</mn><mo>±</mo><mn>1.4</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2143.gif" /></p></td></tr><tr><td align="left"><p>   1.00–1.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>40.3</mn><mo>±</mo><mn>1.2</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2144.gif" /></p></td><td align="left"><p>1.2</p></td><td align="left"><p>1.2</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.7</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.0</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>34.5</mn><mo>±</mo><mn>1.1</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2145.gif" /></p></td></tr><tr><td align="left"><p>   1.50–2.00</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>17.92</mn><mo>±</mo><mn>0.68</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2146.gif" /></p></td><td align="left"><p>1.9</p></td><td align="left"><p>1.7</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.3</p></td><td align="left"><p>1.4</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>15.33</mn><mo>±</mo><mn>0.60</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2147.gif" /></p></td></tr><tr><td align="left"><p>   2.00–2.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3.30</mn><mo>±</mo><mn>0.24</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2148.gif" /></p></td><td align="left"><p>5.3</p></td><td align="left"><p>2.9</p></td><td align="left"><p>1.2</p></td><td align="left"><p>1.1</p></td><td align="left"><p>2.8</p></td><td align="left"><p>2.4</p></td><td align="left"><p>7.3</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.86</mn><mo>±</mo><mn>0.21</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2149.gif" /></p></td></tr><tr><td align="left" colspan="10"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>120</mn><mo><</mo><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mo><</mo><mn>200</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2150.gif" /></p></td></tr><tr><td align="left"><p>   0.00–0.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>33.95</mn><mo>±</mo><mn>0.98</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2151.gif" /></p></td><td align="left"><p>0.8</p></td><td align="left"><p>1.2</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.7</p></td><td align="left"><p>2.3</p></td><td align="left"><p>2.9</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>29.66</mn><mo>±</mo><mn>0.84</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2152.gif" /></p></td></tr><tr><td align="left"><p>   0.50–1.00</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>28.57</mn><mo>±</mo><mn>0.85</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2153.gif" /></p></td><td align="left"><p>0.9</p></td><td align="left"><p>1.3</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.8</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.0</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>25.02</mn><mo>±</mo><mn>0.72</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2154.gif" /></p></td></tr><tr><td align="left"><p>   1.00–1.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>17.01</mn><mo>±</mo><mn>0.56</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2155.gif" /></p></td><td align="left"><p>1.2</p></td><td align="left"><p>1.5</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.2</p></td><td align="left"><p>1.1</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.3</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>14.98</mn><mo>±</mo><mn>0.48</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2156.gif" /></p></td></tr><tr><td align="left"><p>   1.50–2.00</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>6.65</mn><mo>±</mo><mn>0.28</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2157.gif" /></p></td><td align="left"><p>2.1</p></td><td align="left"><p>2.0</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.3</p></td><td align="left"><p>1.6</p></td><td align="left"><p>2.3</p></td><td align="left"><p>4.2</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>5.89</mn><mo>±</mo><mn>0.25</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2158.gif" /></p></td></tr><tr><td align="left"><p>   2.00–2.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.84</mn><mo>±</mo><mn>0.08</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2159.gif" /></p></td><td align="left"><p>7.4</p></td><td align="left"><p>3.6</p></td><td align="left"><p>1.6</p></td><td align="left"><p>1.2</p></td><td align="left"><p>4.2</p></td><td align="left"><p>2.5</p></td><td align="left"><p>9.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.74</mn><mo>±</mo><mn>0.07</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2160.gif" /></p></td></tr><tr><td align="left" colspan="10"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>200</mn><mo><</mo><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mo><</mo><mn>500</mn><mo>+</mo><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2161.gif" /></p></td></tr><tr><td align="left"><p>   0.00–0.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4.85</mn><mo>±</mo><mn>0.18</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2162.gif" /></p></td><td align="left"><p>1.1</p></td><td align="left"><p>1.7</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.3</p></td><td align="left"><p>1.8</p></td><td align="left"><p>2.4</p></td><td align="left"><p>3.6</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4.41</mn><mo>±</mo><mn>0.16</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2163.gif" /></p></td></tr><tr><td align="left"><p>   0.50–1.00</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3.56</mn><mo>±</mo><mn>0.13</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2164.gif" /></p></td><td align="left"><p>1.3</p></td><td align="left"><p>1.2</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.3</p></td><td align="left"><p>1.9</p></td><td align="left"><p>2.4</p></td><td align="left"><p>3.6</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3.25</mn><mo>±</mo><mn>0.11</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2165.gif" /></p></td></tr><tr><td align="left"><p>   1.00–1.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.72</mn><mo>±</mo><mn>0.07</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2166.gif" /></p></td><td align="left"><p>2.0</p></td><td align="left"><p>1.5</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.3</p></td><td align="left"><p>2.1</p></td><td align="left"><p>2.4</p></td><td align="left"><p>4.1</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.57</mn><mo>±</mo><mn>0.06</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2167.gif" /></p></td></tr><tr><td align="left"><p>   1.50–2.00</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.43</mn><mo>±</mo><mn>0.03</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2168.gif" /></p></td><td align="left"><p>4.1</p></td><td align="left"><p>2.6</p></td><td align="left"><p>1.2</p></td><td align="left"><p>0.3</p></td><td align="left"><p>2.9</p></td><td align="left"><p>2.4</p></td><td align="left"><p>6.2</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.40</mn><mo>±</mo><mn>0.02</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2169.gif" /></p></td></tr><tr><td align="left"><p>   2.00–2.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.04</mn><mo>±</mo><mn>0.01</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2170.gif" /></p></td><td align="left"><p>15.9</p></td><td align="left"><p>7.1</p></td><td align="left"><p>2.4</p></td><td align="left"><p>1.5</p></td><td align="left"><p>5.2</p></td><td align="left"><p>2.7</p></td><td align="left"><p>18.6</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.04</mn><mo>±</mo><mn>0.01</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2171.gif" /></p></td></tr></tbody></table> </ephtml> </p> <p>Normalised differential cross-sections as a function of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo></mrow><msup><mi>y</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mrow><mo stretchy="false">|</mo><mo>×</mo></mrow><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math> </ephtml> . The columns show the bin ranges, measured cross-section and total uncertainty, relative statistical uncertainty, relative systematic uncertainties in various categories (see text), total relative uncertainty, and differential cross-section corrected to remove contributions via <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>W</mi><mo stretchy="false">→</mo><mi>τ</mi><mo stretchy="false">→</mo><mi>e</mi><mo stretchy="false">/</mo><mi>μ</mi></mrow></math> </ephtml> decays. Relative uncertainties smaller than 0.05% are indicated by '0.0'. The last bin includes overflows where indicated by the '+' sign</p> <p> <ephtml> <table frame="hsides" rules="groups"><thead><tr><th align="left"><p>Normalised</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mfrac><mn>1</mn><mi>σ</mi></mfrac><msup><mi mathvariant="normal">d</mi><mn>2</mn></msup><mi>σ</mi><mo stretchy="false">/</mo><mi mathvariant="normal">d</mi><mrow><mo stretchy="false">|</mo><msup><mi>y</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mo stretchy="false">|</mo></mrow><mi mathvariant="normal">d</mi><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2174.gif" /></p></th><th align="left"><p>Stat.</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2175.gif" /> mod.</p></th><th align="left"><p>Lept.</p></th><th align="left"><p>Jet/<italic>b</italic></p></th><th align="left"><p>Bkg.</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>L</mi><mo stretchy="false">/</mo><msub><mi>E</mi><mi mathvariant="normal">b</mi></msub></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2176.gif" /></p></th><th align="left"><p>Total</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mfrac><mn>1</mn><mi>σ</mi></mfrac><msup><mi mathvariant="normal">d</mi><mn>2</mn></msup><mi>σ</mi><mo stretchy="false">/</mo><mi mathvariant="normal">d</mi><mrow><mo stretchy="false">|</mo><msup><mi>y</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mo stretchy="false">|</mo></mrow><mi mathvariant="normal">d</mi><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2177.gif" /></p></th></tr><tr><th align="left" /><th align="left" /><th align="left" /><th align="left" /><th align="left" /><th align="left" /><th align="left" /><th align="left" /><th align="left" /><th align="left"><p>(no <math xmlns="http://www.w3.org/1998/Math/MathML"><mi xmlns="">τ</mi></math><inline-graphic href="10052_2020_7907_Article_IEq2178.gif" />)</p></th></tr><tr><th align="left"><p>Bin (unit |<italic>y</italic>| <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2179.gif" />)</p></th><th align="left"><p>(<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msup><mn>10</mn><mrow><mo>-</mo><mn>3</mn></mrow></msup><mo stretchy="false">/</mo><mtext>unit</mtext><mspace width="0.333333em" /><mrow><mo stretchy="false">|</mo><mi>y</mi><mo stretchy="false">|</mo></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2180.gif" /><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2181.gif" />)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msup><mn>10</mn><mrow><mo>-</mo><mn>3</mn></mrow></msup><mo stretchy="false">/</mo></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2182.gif" />unit |<italic>y</italic>| <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2183.gif" />)</p></th></tr></thead><tbody><tr><td align="left" colspan="10"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0</mn><mo><</mo><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mo><</mo><mn>80</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2184.gif" /></p></td></tr><tr><td align="left"><p>   0.00–0.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3.165</mn><mo>±</mo><mn>0.044</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2185.gif" /></p></td><td align="left"><p>0.7</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.4</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3.061</mn><mo>±</mo><mn>0.040</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2186.gif" /></p></td></tr><tr><td align="left"><p>   0.50–1.00</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.733</mn><mo>±</mo><mn>0.035</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2187.gif" /></p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.3</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.649</mn><mo>±</mo><mn>0.032</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2188.gif" /></p></td></tr><tr><td align="left"><p>   1.00–1.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.080</mn><mo>±</mo><mn>0.032</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2189.gif" /></p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.5</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.024</mn><mo>±</mo><mn>0.029</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2190.gif" /></p></td></tr><tr><td align="left"><p>   1.50–2.00</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.226</mn><mo>±</mo><mn>0.027</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2191.gif" /></p></td><td align="left"><p>1.4</p></td><td align="left"><p>1.3</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.0</p></td><td align="left"><p>2.2</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.202</mn><mo>±</mo><mn>0.026</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2192.gif" /></p></td></tr><tr><td align="left"><p>   2.00–2.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.291</mn><mo>±</mo><mn>0.014</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2193.gif" /></p></td><td align="left"><p>3.4</p></td><td align="left"><p>2.3</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.4</p></td><td align="left"><p>2.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>4.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.287</mn><mo>±</mo><mn>0.013</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2194.gif" /></p></td></tr><tr><td align="left" colspan="10"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>80</mn><mo><</mo><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mo><</mo><mn>120</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2195.gif" /></p></td></tr><tr><td align="left"><p>   0.00–0.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4.758</mn><mo>±</mo><mn>0.049</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2196.gif" /></p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.0</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4.696</mn><mo>±</mo><mn>0.048</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2197.gif" /></p></td></tr><tr><td align="left"><p>   0.50–1.00</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4.017</mn><mo>±</mo><mn>0.044</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2198.gif" /></p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.1</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3.974</mn><mo>±</mo><mn>0.045</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2199.gif" /></p></td></tr><tr><td align="left"><p>   1.00–1.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.846</mn><mo>±</mo><mn>0.041</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2200.gif" /></p></td><td align="left"><p>1.1</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.5</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.840</mn><mo>±</mo><mn>0.043</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2201.gif" /></p></td></tr><tr><td align="left"><p>   1.50–2.00</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.264</mn><mo>±</mo><mn>0.031</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2202.gif" /></p></td><td align="left"><p>1.8</p></td><td align="left"><p>1.3</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.0</p></td><td align="left"><p>2.5</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.263</mn><mo>±</mo><mn>0.033</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2203.gif" /></p></td></tr><tr><td align="left"><p>   2.00–2.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.233</mn><mo>±</mo><mn>0.015</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2204.gif" /></p></td><td align="left"><p>5.3</p></td><td align="left"><p>2.6</p></td><td align="left"><p>0.7</p></td><td align="left"><p>1.1</p></td><td align="left"><p>2.5</p></td><td align="left"><p>0.1</p></td><td align="left"><p>6.5</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.236</mn><mo>±</mo><mn>0.016</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2205.gif" /></p></td></tr><tr><td align="left" colspan="10"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>120</mn><mo><</mo><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mo><</mo><mn>200</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2206.gif" /></p></td></tr><tr><td align="left"><p>   0.00–0.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.395</mn><mo>±</mo><mn>0.024</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2207.gif" /></p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.0</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.444</mn><mo>±</mo><mn>0.025</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2208.gif" /></p></td></tr><tr><td align="left"><p>   0.50–1.00</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.016</mn><mo>±</mo><mn>0.024</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2209.gif" /></p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.2</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.062</mn><mo>±</mo><mn>0.023</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2210.gif" /></p></td></tr><tr><td align="left"><p>   1.00–1.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.200</mn><mo>±</mo><mn>0.021</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2211.gif" /></p></td><td align="left"><p>1.2</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.234</mn><mo>±</mo><mn>0.021</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2212.gif" /></p></td></tr><tr><td align="left"><p>   1.50–2.00</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.469</mn><mo>±</mo><mn>0.014</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2213.gif" /></p></td><td align="left"><p>2.1</p></td><td align="left"><p>1.6</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.3</p></td><td align="left"><p>1.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>3.0</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.485</mn><mo>±</mo><mn>0.015</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2214.gif" /></p></td></tr><tr><td align="left"><p>   2.00–2.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.0592</mn><mo>±</mo><mn>0.0054</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2215.gif" /></p></td><td align="left"><p>7.4</p></td><td align="left"><p>3.4</p></td><td align="left"><p>1.3</p></td><td align="left"><p>1.2</p></td><td align="left"><p>3.9</p></td><td align="left"><p>0.2</p></td><td align="left"><p>9.2</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.0611</mn><mo>±</mo><mn>0.0056</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2216.gif" /></p></td></tr><tr><td align="left" colspan="10"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>200</mn><mo><</mo><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mo><</mo><mn>500</mn><mo>+</mo><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2217.gif" /></p></td></tr><tr><td align="left"><p>   0.00–0.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.3425</mn><mo>±</mo><mn>0.0084</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2218.gif" /></p></td><td align="left"><p>1.1</p></td><td align="left"><p>1.5</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.1</p></td><td align="left"><p>1.6</p></td><td align="left"><p>0.0</p></td><td align="left"><p>2.5</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.3634</mn><mo>±</mo><mn>0.0086</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2219.gif" /></p></td></tr><tr><td align="left"><p>   0.50–1.00</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.2513</mn><mo>±</mo><mn>0.0058</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2220.gif" /></p></td><td align="left"><p>1.3</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.3</p></td><td align="left"><p>1.6</p></td><td align="left"><p>0.0</p></td><td align="left"><p>2.3</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.2676</mn><mo>±</mo><mn>0.0061</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2221.gif" /></p></td></tr><tr><td align="left"><p>   1.00–1.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.1211</mn><mo>±</mo><mn>0.0036</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2222.gif" /></p></td><td align="left"><p>2.0</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.1</p></td><td align="left"><p>1.8</p></td><td align="left"><p>0.1</p></td><td align="left"><p>2.9</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.1292</mn><mo>±</mo><mn>0.0038</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2223.gif" /></p></td></tr><tr><td align="left"><p>   1.50–2.00</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.0306</mn><mo>±</mo><mn>0.0017</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2224.gif" /></p></td><td align="left"><p>4.1</p></td><td align="left"><p>2.3</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.3</p></td><td align="left"><p>2.5</p></td><td align="left"><p>0.1</p></td><td align="left"><p>5.4</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.0327</mn><mo>±</mo><mn>0.0018</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2225.gif" /></p></td></tr><tr><td align="left"><p>   2.00–2.50</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.0029</mn><mo>±</mo><mn>0.0005</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2226.gif" /></p></td><td align="left"><p>15.9</p></td><td align="left"><p>6.9</p></td><td align="left"><p>2.1</p></td><td align="left"><p>1.5</p></td><td align="left"><p>4.9</p></td><td align="left"><p>0.4</p></td><td align="left"><p>18.2</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.0031</mn><mo>±</mo><mn>0.0006</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2227.gif" /></p></td></tr></tbody></table> </ephtml> </p> <p>Absolute differential cross-sections as a function of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo><mi mathvariant="normal">Δ</mi></mrow><msup><mi>ϕ</mi><mi>ℓ</mi></msup><mrow><mo stretchy="false">|</mo><mo>×</mo></mrow><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math> </ephtml> . The columns show the bin ranges, measured cross-section and total uncertainty, relative statistical uncertainty, relative systematic uncertainties in various categories (see text), total relative uncertainty, and differential cross-section corrected to remove contributions via <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>W</mi><mo stretchy="false">→</mo><mi>τ</mi><mo stretchy="false">→</mo><mi>e</mi><mo stretchy="false">/</mo><mi>μ</mi></mrow></math> </ephtml> decays. Relative uncertainties smaller than 0.05% are indicated by '0.0'. The bin boundaries for <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi mathvariant="normal">Δ</mi><msup><mi>ϕ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math> </ephtml> correspond to exact multiples of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>π</mi><mo stretchy="false">/</mo><mn>10</mn></mrow></math> </ephtml> but are quoted to two decimal places</p> <p> <ephtml> <table frame="hsides" rules="groups"><thead><tr><th align="left"><p>Absolute</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msup><mi mathvariant="normal">d</mi><mn>2</mn></msup><mi>σ</mi><mo stretchy="false">/</mo><mi mathvariant="normal">d</mi><mi mathvariant="normal">Δ</mi><msup><mi>ϕ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mi mathvariant="normal">d</mi><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2232.gif" /></p></th><th align="left"><p>Stat.</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2233.gif" /> mod.</p></th><th align="left"><p>Lept.</p></th><th align="left"><p>Jet/<italic>b</italic></p></th><th align="left"><p>Bkg.</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>L</mi><mo stretchy="false">/</mo><msub><mi>E</mi><mi mathvariant="normal">b</mi></msub></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2234.gif" /></p></th><th align="left"><p>Total</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msup><mi mathvariant="normal">d</mi><mn>2</mn></msup><mi>σ</mi><mo stretchy="false">/</mo><mi mathvariant="normal">d</mi><mi mathvariant="normal">Δ</mi><msup><mi>ϕ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mi mathvariant="normal">d</mi><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2235.gif" /></p></th></tr><tr><th align="left" /><th align="left" /><th align="left" /><th align="left" /><th align="left" /><th align="left" /><th align="left" /><th align="left" /><th align="left" /><th align="left"><p>(no <math xmlns="http://www.w3.org/1998/Math/MathML"><mi xmlns="">τ</mi></math><inline-graphic href="10052_2020_7907_Article_IEq2236.gif" />)</p></th></tr><tr><th align="left"><p>Bin (rad <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2237.gif" />)</p></th><th align="left"><p>(fb/rad <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2238.gif" />)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(fb/rad <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2239.gif" />)</p></th></tr></thead><tbody><tr><td align="left" colspan="10"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0</mn><mo><</mo><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mo><</mo><mn>80</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2240.gif" /></p></td></tr><tr><td align="left"><p>   0.00–0.31</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>31.2</mn><mo>±</mo><mn>1.0</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2241.gif" /></p></td><td align="left"><p>1.2</p></td><td align="left"><p>1.6</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.1</p></td><td align="left"><p>1.0</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.4</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>27.0</mn><mo>±</mo><mn>0.9</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2242.gif" /></p></td></tr><tr><td align="left"><p>   0.31–0.63</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>31.13</mn><mo>±</mo><mn>0.99</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2243.gif" /></p></td><td align="left"><p>1.1</p></td><td align="left"><p>1.4</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.9</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.2</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>27.04</mn><mo>±</mo><mn>0.82</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2244.gif" /></p></td></tr><tr><td align="left"><p>   0.63–0.94</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>30.34</mn><mo>±</mo><mn>0.95</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2245.gif" /></p></td><td align="left"><p>1.2</p></td><td align="left"><p>1.3</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.9</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.1</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>26.31</mn><mo>±</mo><mn>0.79</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2246.gif" /></p></td></tr><tr><td align="left"><p>   0.94–1.26</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>29.60</mn><mo>±</mo><mn>0.92</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2247.gif" /></p></td><td align="left"><p>1.2</p></td><td align="left"><p>1.1</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.9</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.1</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>25.31</mn><mo>±</mo><mn>0.76</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2248.gif" /></p></td></tr><tr><td align="left"><p>   1.26–1.57</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>25.05</mn><mo>±</mo><mn>0.80</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2249.gif" /></p></td><td align="left"><p>1.3</p></td><td align="left"><p>1.1</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.2</p></td><td align="left"><p>1.0</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.2</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>20.89</mn><mo>±</mo><mn>0.64</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2250.gif" /></p></td></tr><tr><td align="left"><p>   1.57–1.88</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>20.21</mn><mo>±</mo><mn>0.66</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2251.gif" /></p></td><td align="left"><p>1.5</p></td><td align="left"><p>1.1</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.3</p></td><td align="left"><p>1.0</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.3</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>16.31</mn><mo>±</mo><mn>0.52</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2252.gif" /></p></td></tr><tr><td align="left"><p>   1.88–2.20</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>15.63</mn><mo>±</mo><mn>0.55</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2253.gif" /></p></td><td align="left"><p>1.8</p></td><td align="left"><p>1.3</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.2</p></td><td align="left"><p>1.1</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.5</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>12.16</mn><mo>±</mo><mn>0.42</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2254.gif" /></p></td></tr><tr><td align="left"><p>   2.20–2.51</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>12.27</mn><mo>±</mo><mn>0.46</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2255.gif" /></p></td><td align="left"><p>2.1</p></td><td align="left"><p>1.4</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.3</p></td><td align="left"><p>1.1</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>9.27</mn><mo>±</mo><mn>0.34</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2256.gif" /></p></td></tr><tr><td align="left"><p>   2.51–2.83</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>10.07</mn><mo>±</mo><mn>0.40</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2257.gif" /></p></td><td align="left"><p>2.3</p></td><td align="left"><p>1.6</p></td><td align="left"><p>1.1</p></td><td align="left"><p>0.2</p></td><td align="left"><p>1.3</p></td><td align="left"><p>2.3</p></td><td align="left"><p>4.0</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>7.53</mn><mo>±</mo><mn>0.29</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2258.gif" /></p></td></tr><tr><td align="left"><p>   2.83–3.14</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>8.38</mn><mo>±</mo><mn>0.37</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2259.gif" /></p></td><td align="left"><p>2.6</p></td><td align="left"><p>1.8</p></td><td align="left"><p>1.1</p></td><td align="left"><p>0.6</p></td><td align="left"><p>1.7</p></td><td align="left"><p>2.3</p></td><td align="left"><p>4.4</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>6.20</mn><mo>±</mo><mn>0.27</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2260.gif" /></p></td></tr><tr><td align="left" colspan="10"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>80</mn><mo><</mo><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mo><</mo><mn>120</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2261.gif" /></p></td></tr><tr><td align="left"><p>   0.00–0.31</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>10.11</mn><mo>±</mo><mn>0.44</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2262.gif" /></p></td><td align="left"><p>2.8</p></td><td align="left"><p>1.9</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.4</p></td><td align="left"><p>1.3</p></td><td align="left"><p>2.3</p></td><td align="left"><p>4.3</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>9.13</mn><mo>±</mo><mn>0.40</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2263.gif" /></p></td></tr><tr><td align="left"><p>   0.31–0.63</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>10.92</mn><mo>±</mo><mn>0.45</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2264.gif" /></p></td><td align="left"><p>2.6</p></td><td align="left"><p>1.7</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.4</p></td><td align="left"><p>1.0</p></td><td align="left"><p>2.3</p></td><td align="left"><p>4.1</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>9.84</mn><mo>±</mo><mn>0.40</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2265.gif" /></p></td></tr><tr><td align="left"><p>   0.63–0.94</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>13.61</mn><mo>±</mo><mn>0.52</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2266.gif" /></p></td><td align="left"><p>2.3</p></td><td align="left"><p>1.5</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.4</p></td><td align="left"><p>1.0</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>12.28</mn><mo>±</mo><mn>0.46</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2267.gif" /></p></td></tr><tr><td align="left"><p>   0.94–1.26</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>19.44</mn><mo>±</mo><mn>0.68</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2268.gif" /></p></td><td align="left"><p>1.9</p></td><td align="left"><p>1.3</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.9</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.5</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>17.50</mn><mo>±</mo><mn>0.60</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2269.gif" /></p></td></tr><tr><td align="left"><p>   1.26–1.57</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>29.17</mn><mo>±</mo><mn>0.94</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2270.gif" /></p></td><td align="left"><p>1.6</p></td><td align="left"><p>1.1</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.9</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.2</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>26.19</mn><mo>±</mo><mn>0.83</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2271.gif" /></p></td></tr><tr><td align="left"><p>   1.57–1.88</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>38.7</mn><mo>±</mo><mn>1.2</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2272.gif" /></p></td><td align="left"><p>1.4</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.8</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.1</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>34.1</mn><mo>±</mo><mn>1.0</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2273.gif" /></p></td></tr><tr><td align="left"><p>   1.88–2.20</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>44.6</mn><mo>±</mo><mn>1.4</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2274.gif" /></p></td><td align="left"><p>1.3</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.8</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.1</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>37.9</mn><mo>±</mo><mn>1.1</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2275.gif" /></p></td></tr><tr><td align="left"><p>   2.20–2.51</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>45.4</mn><mo>±</mo><mn>1.4</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2276.gif" /></p></td><td align="left"><p>1.3</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.8</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.0</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>37.3</mn><mo>±</mo><mn>1.1</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2277.gif" /></p></td></tr><tr><td align="left"><p>   2.51–2.83</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>42.5</mn><mo>±</mo><mn>1.3</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2278.gif" /></p></td><td align="left"><p>1.4</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.8</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.1</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>34.1</mn><mo>±</mo><mn>1.1</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2279.gif" /></p></td></tr><tr><td align="left"><p>   2.83–3.14</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>41.8</mn><mo>±</mo><mn>1.3</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2280.gif" /></p></td><td align="left"><p>1.4</p></td><td align="left"><p>1.1</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.8</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.1</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>33.1</mn><mo>±</mo><mn>1.1</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2281.gif" /></p></td></tr><tr><td align="left" colspan="10"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>120</mn><mo><</mo><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mo><</mo><mn>200</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2282.gif" /></p></td></tr><tr><td align="left"><p>   0.00–0.31</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3.44</mn><mo>±</mo><mn>0.22</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2283.gif" /></p></td><td align="left"><p>3.3</p></td><td align="left"><p>4.8</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.3</p></td><td align="left"><p>1.3</p></td><td align="left"><p>2.3</p></td><td align="left"><p>6.5</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3.17</mn><mo>±</mo><mn>0.21</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2284.gif" /></p></td></tr><tr><td align="left"><p>   0.31–0.63</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3.33</mn><mo>±</mo><mn>0.20</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2285.gif" /></p></td><td align="left"><p>3.3</p></td><td align="left"><p>4.1</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.2</p></td><td align="left"><p>1.3</p></td><td align="left"><p>2.3</p></td><td align="left"><p>6.0</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3.05</mn><mo>±</mo><mn>0.19</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2286.gif" /></p></td></tr><tr><td align="left"><p>   0.63–0.94</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3.92</mn><mo>±</mo><mn>0.21</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2287.gif" /></p></td><td align="left"><p>3.1</p></td><td align="left"><p>3.4</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.5</p></td><td align="left"><p>1.5</p></td><td align="left"><p>2.3</p></td><td align="left"><p>5.5</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3.59</mn><mo>±</mo><mn>0.20</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2288.gif" /></p></td></tr><tr><td align="left"><p>   0.94–1.26</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>5.41</mn><mo>±</mo><mn>0.25</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2289.gif" /></p></td><td align="left"><p>2.6</p></td><td align="left"><p>2.7</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.2</p></td><td align="left"><p>1.2</p></td><td align="left"><p>2.3</p></td><td align="left"><p>4.6</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4.94</mn><mo>±</mo><mn>0.24</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2290.gif" /></p></td></tr><tr><td align="left"><p>   1.26–1.57</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>8.28</mn><mo>±</mo><mn>0.32</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2291.gif" /></p></td><td align="left"><p>2.1</p></td><td align="left"><p>2.0</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.4</p></td><td align="left"><p>1.0</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.9</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>7.55</mn><mo>±</mo><mn>0.31</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2292.gif" /></p></td></tr><tr><td align="left"><p>   1.57–1.88</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>12.70</mn><mo>±</mo><mn>0.44</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2293.gif" /></p></td><td align="left"><p>1.7</p></td><td align="left"><p>1.5</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.2</p></td><td align="left"><p>1.0</p></td><td align="left"><p>2.4</p></td><td align="left"><p>3.5</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>11.52</mn><mo>±</mo><mn>0.40</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2294.gif" /></p></td></tr><tr><td align="left"><p>   1.88–2.20</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>18.44</mn><mo>±</mo><mn>0.59</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2295.gif" /></p></td><td align="left"><p>1.4</p></td><td align="left"><p>1.3</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.9</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.2</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>16.55</mn><mo>±</mo><mn>0.52</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2296.gif" /></p></td></tr><tr><td align="left"><p>   2.20–2.51</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>24.92</mn><mo>±</mo><mn>0.80</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2297.gif" /></p></td><td align="left"><p>1.2</p></td><td align="left"><p>1.5</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.8</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.2</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>21.86</mn><mo>±</mo><mn>0.68</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2298.gif" /></p></td></tr><tr><td align="left"><p>   2.51–2.83</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>28.48</mn><mo>±</mo><mn>0.99</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2299.gif" /></p></td><td align="left"><p>1.2</p></td><td align="left"><p>2.0</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.8</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.5</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>24.35</mn><mo>±</mo><mn>0.85</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2300.gif" /></p></td></tr><tr><td align="left"><p>   2.83–3.14</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>29.7</mn><mo>±</mo><mn>1.1</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2301.gif" /></p></td><td align="left"><p>1.1</p></td><td align="left"><p>2.7</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.8</p></td><td align="left"><p>2.3</p></td><td align="left"><p>3.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>25.0</mn><mo>±</mo><mn>1.0</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2302.gif" /></p></td></tr><tr><td align="left" colspan="10"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>200</mn><mo><</mo><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mo><</mo><mn>500</mn><mo>+</mo><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2303.gif" /></p></td></tr><tr><td align="left"><p>   0.00–0.31</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.23</mn><mo>±</mo><mn>0.03</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2304.gif" /></p></td><td align="left"><p>7.1</p></td><td align="left"><p>6.3</p></td><td align="left"><p>0.9</p></td><td align="left"><p>1.0</p></td><td align="left"><p>5.6</p></td><td align="left"><p>2.3</p></td><td align="left"><p>11.4</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.22</mn><mo>±</mo><mn>0.02</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2305.gif" /></p></td></tr><tr><td align="left"><p>   0.31–0.63</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.30</mn><mo>±</mo><mn>0.03</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2306.gif" /></p></td><td align="left"><p>6.3</p></td><td align="left"><p>5.6</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.7</p></td><td align="left"><p>4.3</p></td><td align="left"><p>2.3</p></td><td align="left"><p>9.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.28</mn><mo>±</mo><mn>0.03</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2307.gif" /></p></td></tr><tr><td align="left"><p>   0.63–0.94</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.29</mn><mo>±</mo><mn>0.03</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2308.gif" /></p></td><td align="left"><p>6.2</p></td><td align="left"><p>4.8</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.8</p></td><td align="left"><p>5.0</p></td><td align="left"><p>2.4</p></td><td align="left"><p>9.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.27</mn><mo>±</mo><mn>0.03</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2309.gif" /></p></td></tr><tr><td align="left"><p>   0.94–1.26</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.36</mn><mo>±</mo><mn>0.03</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2310.gif" /></p></td><td align="left"><p>5.6</p></td><td align="left"><p>3.9</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.8</p></td><td align="left"><p>3.7</p></td><td align="left"><p>2.3</p></td><td align="left"><p>8.2</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.34</mn><mo>±</mo><mn>0.03</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2311.gif" /></p></td></tr><tr><td align="left"><p>   1.26–1.57</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.54</mn><mo>±</mo><mn>0.04</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2312.gif" /></p></td><td align="left"><p>4.3</p></td><td align="left"><p>3.1</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.5</p></td><td align="left"><p>3.2</p></td><td align="left"><p>2.4</p></td><td align="left"><p>6.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.51</mn><mo>±</mo><mn>0.03</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2313.gif" /></p></td></tr><tr><td align="left"><p>   1.57–1.88</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.93</mn><mo>±</mo><mn>0.05</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2314.gif" /></p></td><td align="left"><p>3.3</p></td><td align="left"><p>2.4</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.4</p></td><td align="left"><p>2.7</p></td><td align="left"><p>2.3</p></td><td align="left"><p>5.5</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.87</mn><mo>±</mo><mn>0.05</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2315.gif" /></p></td></tr><tr><td align="left"><p>   1.88–2.20</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.60</mn><mo>±</mo><mn>0.07</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2316.gif" /></p></td><td align="left"><p>2.4</p></td><td align="left"><p>1.7</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.5</p></td><td align="left"><p>2.1</p></td><td align="left"><p>2.3</p></td><td align="left"><p>4.4</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.48</mn><mo>±</mo><mn>0.07</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2317.gif" /></p></td></tr><tr><td align="left"><p>   2.20–2.51</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.76</mn><mo>±</mo><mn>0.11</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2318.gif" /></p></td><td align="left"><p>1.9</p></td><td align="left"><p>1.4</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.4</p></td><td align="left"><p>1.9</p></td><td align="left"><p>2.4</p></td><td align="left"><p>3.9</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.54</mn><mo>±</mo><mn>0.10</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2319.gif" /></p></td></tr><tr><td align="left"><p>   2.51–2.83</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>4.22</mn><mo>±</mo><mn>0.16</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2320.gif" /></p></td><td align="left"><p>1.5</p></td><td align="left"><p>1.5</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.3</p></td><td align="left"><p>1.7</p></td><td align="left"><p>2.4</p></td><td align="left"><p>3.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3.83</mn><mo>±</mo><mn>0.14</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2321.gif" /></p></td></tr><tr><td align="left"><p>   2.83–3.14</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>5.68</mn><mo>±</mo><mn>0.21</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2322.gif" /></p></td><td align="left"><p>1.3</p></td><td align="left"><p>2.0</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.3</p></td><td align="left"><p>1.3</p></td><td align="left"><p>2.4</p></td><td align="left"><p>3.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>5.08</mn><mo>±</mo><mn>0.18</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2323.gif" /></p></td></tr></tbody></table> </ephtml> </p> <p>Normalised differential cross-sections as a function of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mrow><mo stretchy="false">|</mo><mi mathvariant="normal">Δ</mi></mrow><msup><mi>ϕ</mi><mi>ℓ</mi></msup><mrow><mo stretchy="false">|</mo><mo>×</mo></mrow><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math> </ephtml> . The columns show the bin ranges, measured cross-section and total uncertainty, relative statistical uncertainty, relative systematic uncertainties in various categories (see text), total relative uncertainty, and differential cross-section corrected to remove contributions via <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>W</mi><mo stretchy="false">→</mo><mi>τ</mi><mo stretchy="false">→</mo><mi>e</mi><mo stretchy="false">/</mo><mi>μ</mi></mrow></math> </ephtml> decays. Relative uncertainties smaller than 0.05% are indicated by '0.0'. The bin boundaries for <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi mathvariant="normal">Δ</mi><msup><mi>ϕ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math> </ephtml> correspond to exact multiples of <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>π</mi><mo stretchy="false">/</mo><mn>10</mn></mrow></math> </ephtml> but are quoted to two decimal places</p> <p> <ephtml> <table frame="hsides" rules="groups"><thead><tr><th align="left"><p>Normalised</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mfrac><mn>1</mn><mi>σ</mi></mfrac><msup><mi mathvariant="normal">d</mi><mn>2</mn></msup><mi>σ</mi><mo stretchy="false">/</mo><mi mathvariant="normal">d</mi><mi mathvariant="normal">Δ</mi><msup><mi>ϕ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mi mathvariant="normal">d</mi><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2328.gif" /></p></th><th align="left"><p>Stat.</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2329.gif" /> mod.</p></th><th align="left"><p>Lept.</p></th><th align="left"><p>Jet/<italic>b</italic></p></th><th align="left"><p>Bkg.</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mi>L</mi><mo stretchy="false">/</mo><msub><mi>E</mi><mi mathvariant="normal">b</mi></msub></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2330.gif" /></p></th><th align="left"><p>Total</p></th><th align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mfrac><mn>1</mn><mi>σ</mi></mfrac><msup><mi mathvariant="normal">d</mi><mn>2</mn></msup><mi>σ</mi><mo stretchy="false">/</mo><mi mathvariant="normal">d</mi><mi mathvariant="normal">Δ</mi><msup><mi>ϕ</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mi mathvariant="normal">d</mi><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2331.gif" /></p></th></tr><tr><th align="left" /><th align="left" /><th align="left" /><th align="left" /><th align="left" /><th align="left" /><th align="left" /><th align="left" /><th align="left" /><th align="left"><p>(no <math xmlns="http://www.w3.org/1998/Math/MathML"><mi xmlns="">τ</mi></math><inline-graphic href="10052_2020_7907_Article_IEq2332.gif" />)</p></th></tr><tr><th align="left"><p>Bin (rad <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2333.gif" />)</p></th><th align="left"><p>(<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msup><mn>10</mn><mrow><mo>-</mo><mn>3</mn></mrow></msup><mo stretchy="false">/</mo></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2334.gif" />rad <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2335.gif" />)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(%)</p></th><th align="left"><p>(<math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><msup><mn>10</mn><mrow><mo>-</mo><mn>3</mn></mrow></msup><mo stretchy="false">/</mo></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2336.gif" />rad <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2337.gif" />)</p></th></tr></thead><tbody><tr><td align="left" colspan="10"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0</mn><mo><</mo><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mo><</mo><mn>80</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2338.gif" /></p></td></tr><tr><td align="left"><p>   0.00–0.31</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.204</mn><mo>±</mo><mn>0.047</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2339.gif" /></p></td><td align="left"><p>1.2</p></td><td align="left"><p>1.6</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.0</p></td><td align="left"><p>2.1</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.224</mn><mo>±</mo><mn>0.045</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2340.gif" /></p></td></tr><tr><td align="left"><p>   0.31–0.63</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.196</mn><mo>±</mo><mn>0.041</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2341.gif" /></p></td><td align="left"><p>1.1</p></td><td align="left"><p>1.3</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.227</mn><mo>±</mo><mn>0.038</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2342.gif" /></p></td></tr><tr><td align="left"><p>   0.63–0.94</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.140</mn><mo>±</mo><mn>0.036</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2343.gif" /></p></td><td align="left"><p>1.1</p></td><td align="left"><p>1.1</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.167</mn><mo>±</mo><mn>0.034</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2344.gif" /></p></td></tr><tr><td align="left"><p>   0.94–1.26</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.088</mn><mo>±</mo><mn>0.033</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2345.gif" /></p></td><td align="left"><p>1.2</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.6</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.084</mn><mo>±</mo><mn>0.032</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2346.gif" /></p></td></tr><tr><td align="left"><p>   1.26–1.57</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.767</mn><mo>±</mo><mn>0.029</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2347.gif" /></p></td><td align="left"><p>1.3</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.720</mn><mo>±</mo><mn>0.028</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2348.gif" /></p></td></tr><tr><td align="left"><p>   1.57–1.88</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.426</mn><mo>±</mo><mn>0.026</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2349.gif" /></p></td><td align="left"><p>1.5</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.343</mn><mo>±</mo><mn>0.024</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2350.gif" /></p></td></tr><tr><td align="left"><p>   1.88–2.20</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.103</mn><mo>±</mo><mn>0.023</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2351.gif" /></p></td><td align="left"><p>1.7</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.0</p></td><td align="left"><p>2.1</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.001</mn><mo>±</mo><mn>0.022</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2352.gif" /></p></td></tr><tr><td align="left"><p>   2.20–2.51</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.865</mn><mo>±</mo><mn>0.021</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2353.gif" /></p></td><td align="left"><p>2.0</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.0</p></td><td align="left"><p>2.5</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.763</mn><mo>±</mo><mn>0.019</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2354.gif" /></p></td></tr><tr><td align="left"><p>   2.51–2.83</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.710</mn><mo>±</mo><mn>0.020</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2355.gif" /></p></td><td align="left"><p>2.3</p></td><td align="left"><p>1.2</p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.2</p></td><td align="left"><p>1.1</p></td><td align="left"><p>0.1</p></td><td align="left"><p>2.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.620</mn><mo>±</mo><mn>0.018</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2356.gif" /></p></td></tr><tr><td align="left"><p>   2.83–3.14</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.591</mn><mo>±</mo><mn>0.020</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2357.gif" /></p></td><td align="left"><p>2.5</p></td><td align="left"><p>1.4</p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.5</p></td><td align="left"><p>1.5</p></td><td align="left"><p>0.0</p></td><td align="left"><p>3.3</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.511</mn><mo>±</mo><mn>0.017</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2358.gif" /></p></td></tr><tr><td align="left" colspan="10"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>80</mn><mo><</mo><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mo><</mo><mn>120</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2359.gif" /></p></td></tr><tr><td align="left"><p>   0.00–0.31</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.713</mn><mo>±</mo><mn>0.023</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2360.gif" /></p></td><td align="left"><p>2.7</p></td><td align="left"><p>1.4</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.3</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.0</p></td><td align="left"><p>3.3</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.751</mn><mo>±</mo><mn>0.026</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2361.gif" /></p></td></tr><tr><td align="left"><p>   0.31–0.63</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.770</mn><mo>±</mo><mn>0.023</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2362.gif" /></p></td><td align="left"><p>2.6</p></td><td align="left"><p>1.3</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.0</p></td><td align="left"><p>3.0</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.810</mn><mo>±</mo><mn>0.025</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2363.gif" /></p></td></tr><tr><td align="left"><p>   0.63–0.94</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.960</mn><mo>±</mo><mn>0.026</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2364.gif" /></p></td><td align="left"><p>2.3</p></td><td align="left"><p>1.1</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.0</p></td><td align="left"><p>2.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.011</mn><mo>±</mo><mn>0.027</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2365.gif" /></p></td></tr><tr><td align="left"><p>   0.94–1.26</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.371</mn><mo>±</mo><mn>0.030</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2366.gif" /></p></td><td align="left"><p>1.9</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.0</p></td><td align="left"><p>2.2</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.441</mn><mo>±</mo><mn>0.031</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2367.gif" /></p></td></tr><tr><td align="left"><p>   1.26–1.57</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.057</mn><mo>±</mo><mn>0.037</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2368.gif" /></p></td><td align="left"><p>1.6</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.156</mn><mo>±</mo><mn>0.038</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2369.gif" /></p></td></tr><tr><td align="left"><p>   1.57–1.88</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.729</mn><mo>±</mo><mn>0.042</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2370.gif" /></p></td><td align="left"><p>1.4</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.5</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.809</mn><mo>±</mo><mn>0.043</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2371.gif" /></p></td></tr><tr><td align="left"><p>   1.88–2.20</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3.145</mn><mo>±</mo><mn>0.049</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2372.gif" /></p></td><td align="left"><p>1.3</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.6</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3.124</mn><mo>±</mo><mn>0.048</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2373.gif" /></p></td></tr><tr><td align="left"><p>   2.20–2.51</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3.201</mn><mo>±</mo><mn>0.052</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2374.gif" /></p></td><td align="left"><p>1.3</p></td><td align="left"><p>0.8</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.6</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>3.075</mn><mo>±</mo><mn>0.050</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2375.gif" /></p></td></tr><tr><td align="left"><p>   2.51–2.83</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.998</mn><mo>±</mo><mn>0.053</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2376.gif" /></p></td><td align="left"><p>1.4</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.811</mn><mo>±</mo><mn>0.051</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2377.gif" /></p></td></tr><tr><td align="left"><p>   2.83–3.14</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.948</mn><mo>±</mo><mn>0.056</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2378.gif" /></p></td><td align="left"><p>1.4</p></td><td align="left"><p>1.1</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.9</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.722</mn><mo>±</mo><mn>0.058</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2379.gif" /></p></td></tr><tr><td align="left" colspan="10"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>120</mn><mo><</mo><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mo><</mo><mn>200</mn><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2380.gif" /></p></td></tr><tr><td align="left"><p>   0.00–0.31</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.243</mn><mo>±</mo><mn>0.014</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2381.gif" /></p></td><td align="left"><p>3.3</p></td><td align="left"><p>4.7</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.4</p></td><td align="left"><p>1.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>5.9</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.261</mn><mo>±</mo><mn>0.016</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2382.gif" /></p></td></tr><tr><td align="left"><p>   0.31–0.63</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.235</mn><mo>±</mo><mn>0.012</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2383.gif" /></p></td><td align="left"><p>3.3</p></td><td align="left"><p>3.9</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.3</p></td><td align="left"><p>1.2</p></td><td align="left"><p>0.0</p></td><td align="left"><p>5.3</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.251</mn><mo>±</mo><mn>0.014</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2384.gif" /></p></td></tr><tr><td align="left"><p>   0.63–0.94</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.276</mn><mo>±</mo><mn>0.013</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2385.gif" /></p></td><td align="left"><p>3.1</p></td><td align="left"><p>3.2</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.4</p></td><td align="left"><p>1.3</p></td><td align="left"><p>0.0</p></td><td align="left"><p>4.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.296</mn><mo>±</mo><mn>0.015</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2386.gif" /></p></td></tr><tr><td align="left"><p>   0.94–1.26</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.382</mn><mo>±</mo><mn>0.014</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2387.gif" /></p></td><td align="left"><p>2.6</p></td><td align="left"><p>2.4</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.9</p></td><td align="left"><p>0.0</p></td><td align="left"><p>3.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.407</mn><mo>±</mo><mn>0.017</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2388.gif" /></p></td></tr><tr><td align="left"><p>   1.26–1.57</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.584</mn><mo>±</mo><mn>0.016</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2389.gif" /></p></td><td align="left"><p>2.1</p></td><td align="left"><p>1.7</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.0</p></td><td align="left"><p>2.8</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.621</mn><mo>±</mo><mn>0.020</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2390.gif" /></p></td></tr><tr><td align="left"><p>   1.57–1.88</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.896</mn><mo>±</mo><mn>0.018</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2391.gif" /></p></td><td align="left"><p>1.7</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.0</p></td><td align="left"><p>2.0</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.948</mn><mo>±</mo><mn>0.022</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2392.gif" /></p></td></tr><tr><td align="left"><p>   1.88–2.20</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.300</mn><mo>±</mo><mn>0.021</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2393.gif" /></p></td><td align="left"><p>1.3</p></td><td align="left"><p>0.7</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.6</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.363</mn><mo>±</mo><mn>0.022</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2394.gif" /></p></td></tr><tr><td align="left"><p>   2.20–2.51</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.758</mn><mo>±</mo><mn>0.029</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2395.gif" /></p></td><td align="left"><p>1.2</p></td><td align="left"><p>1.1</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.0</p></td><td align="left"><p>1.6</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>1.800</mn><mo>±</mo><mn>0.028</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2396.gif" /></p></td></tr><tr><td align="left"><p>   2.51–2.83</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.009</mn><mo>±</mo><mn>0.042</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2397.gif" /></p></td><td align="left"><p>1.1</p></td><td align="left"><p>1.7</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.0</p></td><td align="left"><p>2.1</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.005</mn><mo>±</mo><mn>0.043</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2398.gif" /></p></td></tr><tr><td align="left"><p>   2.83–3.14</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.095</mn><mo>±</mo><mn>0.057</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2399.gif" /></p></td><td align="left"><p>1.1</p></td><td align="left"><p>2.5</p></td><td align="left"><p>0.2</p></td><td align="left"><p>0.1</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.0</p></td><td align="left"><p>2.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>2.062</mn><mo>±</mo><mn>0.063</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2400.gif" /></p></td></tr><tr><td align="left" colspan="10"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>200</mn><mo><</mo><msup><mi>m</mi><mrow><mi>e</mi><mi>μ</mi></mrow></msup><mo><</mo><mn>500</mn><mo>+</mo><mspace width="0.166667em" /><mrow><mtext>Ge</mtext><mspace width="0.333333em" /></mrow></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2401.gif" /></p></td></tr><tr><td align="left"><p>   0.00–0.31</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.0164</mn><mo>±</mo><mn>0.0018</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2402.gif" /></p></td><td align="left"><p>7.1</p></td><td align="left"><p>6.0</p></td><td align="left"><p>0.7</p></td><td align="left"><p>1.0</p></td><td align="left"><p>5.5</p></td><td align="left"><p>0.0</p></td><td align="left"><p>10.9</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.0179</mn><mo>±</mo><mn>0.0020</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2403.gif" /></p></td></tr><tr><td align="left"><p>   0.31–0.63</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.0209</mn><mo>±</mo><mn>0.0019</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2404.gif" /></p></td><td align="left"><p>6.3</p></td><td align="left"><p>5.3</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.7</p></td><td align="left"><p>4.1</p></td><td align="left"><p>0.0</p></td><td align="left"><p>9.2</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.0227</mn><mo>±</mo><mn>0.0021</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2405.gif" /></p></td></tr><tr><td align="left"><p>   0.63–0.94</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.0205</mn><mo>±</mo><mn>0.0019</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2406.gif" /></p></td><td align="left"><p>6.1</p></td><td align="left"><p>4.5</p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.8</p></td><td align="left"><p>4.9</p></td><td align="left"><p>0.1</p></td><td align="left"><p>9.1</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.0224</mn><mo>±</mo><mn>0.0021</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2407.gif" /></p></td></tr><tr><td align="left"><p>   0.94–1.26</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.0255</mn><mo>±</mo><mn>0.0019</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2408.gif" /></p></td><td align="left"><p>5.6</p></td><td align="left"><p>3.6</p></td><td align="left"><p>0.3</p></td><td align="left"><p>0.8</p></td><td align="left"><p>3.5</p></td><td align="left"><p>0.0</p></td><td align="left"><p>7.6</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.0279</mn><mo>±</mo><mn>0.0022</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2409.gif" /></p></td></tr><tr><td align="left"><p>   1.26–1.57</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.0382</mn><mo>±</mo><mn>0.0023</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2410.gif" /></p></td><td align="left"><p>4.2</p></td><td align="left"><p>2.8</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.6</p></td><td align="left"><p>3.1</p></td><td align="left"><p>0.0</p></td><td align="left"><p>6.0</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.0416</mn><mo>±</mo><mn>0.0026</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2411.gif" /></p></td></tr><tr><td align="left"><p>   1.57–1.88</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.0659</mn><mo>±</mo><mn>0.0031</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2412.gif" /></p></td><td align="left"><p>3.3</p></td><td align="left"><p>2.0</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.2</p></td><td align="left"><p>2.5</p></td><td align="left"><p>0.0</p></td><td align="left"><p>4.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.0717</mn><mo>±</mo><mn>0.0034</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2413.gif" /></p></td></tr><tr><td align="left"><p>   1.88–2.20</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.1130</mn><mo>±</mo><mn>0.0039</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2414.gif" /></p></td><td align="left"><p>2.4</p></td><td align="left"><p>1.3</p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.4</p></td><td align="left"><p>2.0</p></td><td align="left"><p>0.0</p></td><td align="left"><p>3.4</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.1221</mn><mo>±</mo><mn>0.0043</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2415.gif" /></p></td></tr><tr><td align="left"><p>   2.20–2.51</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.1949</mn><mo>±</mo><mn>0.0053</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2416.gif" /></p></td><td align="left"><p>1.8</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.6</p></td><td align="left"><p>0.2</p></td><td align="left"><p>1.7</p></td><td align="left"><p>0.0</p></td><td align="left"><p>2.7</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.2094</mn><mo>±</mo><mn>0.0056</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2417.gif" /></p></td></tr><tr><td align="left"><p>   2.51–2.83</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.2974</mn><mo>±</mo><mn>0.0075</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2418.gif" /></p></td><td align="left"><p>1.5</p></td><td align="left"><p>1.3</p></td><td align="left"><p>0.5</p></td><td align="left"><p>0.3</p></td><td align="left"><p>1.5</p></td><td align="left"><p>0.1</p></td><td align="left"><p>2.5</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.3154</mn><mo>±</mo><mn>0.0075</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2419.gif" /></p></td></tr><tr><td align="left"><p>   2.83–3.14</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.401</mn><mo>±</mo><mn>0.011</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2420.gif" /></p></td><td align="left"><p>1.3</p></td><td align="left"><p>2.0</p></td><td align="left"><p>0.4</p></td><td align="left"><p>0.1</p></td><td align="left"><p>1.0</p></td><td align="left"><p>0.1</p></td><td align="left"><p>2.6</p></td><td align="left"><p><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow xmlns=""><mn>0.418</mn><mo>±</mo><mn>0.010</mn></mrow></math><inline-graphic href="10052_2020_7907_Article_IEq2421.gif" /></p></td></tr></tbody></table> </ephtml> </p> <ref id="AN0144642803-27"> <title> References </title> <blist> <bibl id="bib1" idref="ref1" type="bt">1</bibl> <bibtext> Cacciari M, Czakon M, Mangano M, Mitov A, Nason P. 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The PDF uncertainty envelope was defined to cover the positive and negative 68% confidence level uncertainties of each considered PDF set, and the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>σ</mi><mrow><mi>t</mi><mover accent="true"><mrow><mi>t</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></msub></math> </ephtml> central value was defined as the midpoint of the envelope. The recommended <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>α</mi><mi mathvariant="normal">S</mi></msub></math> </ephtml> value was used for each PDF set ( <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mn>0.1170</mn><mo>±</mo><mn>0.0014</mn></mrow></math> </ephtml> for MSTW2008 and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mn>0.1180</mn><mo>±</mo><mn>0.0012</mn></mrow></math> </ephtml> for CT10 and NNPDF2.3) and the <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>α</mi><mi mathvariant="normal">S</mi></msub></math> </ephtml> variations were included in the envelope uncertainties.</bibtext> </blist> <blist> <bibtext> Charge-conjugate decay modes are implied unless otherwise stated.</bibtext> </blist> <blist> <bibtext> ATLAS uses a right-handed coordinate system with its origin at the nominal interaction point in the centre of the detector, and the <emph>z</emph> axis along the beam line. Pseudorapidity is defined in terms of the polar angle <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mi>θ</mi></math> </ephtml> as <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>η</mi><mo>=</mo><mo>-</mo><mo>ln</mo><mo>tan</mo><mrow><mi>θ</mi><mo stretchy="false">/</mo><mn>2</mn></mrow></mrow></math> </ephtml> , and transverse momentum and energy are defined relative to the beam line as <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>p</mi><mi mathvariant="normal">T</mi></msub><mo>=</mo><mi>p</mi><mo>sin</mo><mi>θ</mi></mrow></math> </ephtml> and <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>E</mi><mi mathvariant="normal">T</mi></msub><mo>=</mo><mi>E</mi><mo>sin</mo><mi>θ</mi></mrow></math> </ephtml> . The azimuthal angle around the beam line is denoted by <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mi>ϕ</mi></math> </ephtml> , and distances in <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mo stretchy="false">(</mo><mi>η</mi><mo>,</mo><mi>ϕ</mi><mo stretchy="false">)</mo></mrow></math> </ephtml> space by <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi mathvariant="normal">Δ</mi><mi>R</mi><mo>=</mo><msqrt><mrow><msup><mrow><mo stretchy="false">(</mo><mi mathvariant="normal">Δ</mi><mi>η</mi><mo stretchy="false">)</mo></mrow><mn>2</mn></msup><mo>+</mo><msup><mrow><mo stretchy="false">(</mo><mi mathvariant="normal">Δ</mi><mi>ϕ</mi><mo stretchy="false">)</mo></mrow><mn>2</mn></msup></mrow></msqrt></mrow></math> </ephtml> . The rapidity is defined as <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>y</mi><mo>=</mo><mfrac><mn>1</mn><mn>2</mn></mfrac><mo>ln</mo><mfenced close=")" open="(" separators=""><mfrac><mrow><mi>E</mi><mo>+</mo><msub><mi>p</mi><mi>z</mi></msub></mrow><mrow><mi>E</mi><mo>-</mo><msub><mi>p</mi><mi>z</mi></msub></mrow></mfrac></mfenced></mrow></math> </ephtml> , where <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>p</mi><mi>z</mi></msub></math> </ephtml> is the <emph>z</emph>-component of the momentum and <emph>E</emph> is the energy of the relevant object or system. The distance in <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mo stretchy="false">(</mo><mi>y</mi><mo>,</mo><mi>ϕ</mi><mo stretchy="false">)</mo></mrow></math> </ephtml> space is given by <ephtml> <math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi mathvariant="normal">Δ</mi><msub><mi>R</mi><mi>y</mi></msub><mo>=</mo><msqrt><mrow><msup><mrow><mo stretchy="false">(</mo><mi mathvariant="normal">Δ</mi><mi>y</mi><mo stretchy="false">)</mo></mrow><mn>2</mn></msup><mo>+</mo><msup><mrow><mo stretchy="false">(</mo><mi mathvariant="normal">Δ</mi><mi>ϕ</mi><mo stretchy="false">)</mo></mrow><mn>2</mn></msup></mrow></msqrt></mrow></math> </ephtml> .</bibtext> </blist> </ref> <aug> <p>By G. Aad; B. Abbott; D. C. Abbott; A. Abed Abud; K. Abeling; D. K. Abhayasinghe; S. H. Abidi; O. S. AbouZeid; N. L. Abraham; H. Abramowicz; H. Abreu; Y. Abulaiti; B. S. Acharya; B. Achkar; S. Adachi; L. Adam; C. Adam Bourdarios; L. Adamczyk; L. Adamek; J. Adelman; M. Adersberger; A. 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Calvet; S. Calvet; T. P. Calvet; M. Calvetti; R. Camacho Toro; S. Camarda; D. Camarero Munoz; P. Camarri; D. Cameron; R. Caminal Armadans; C. Camincher; S. Campana; M. Campanelli; A. Camplani; A. Campoverde; V. Canale; A. Canesse; M. Cano Bret; J. Cantero; T. Cao; Y. Cao; M. D. M. Capeans Garrido; M. Capua; R. Cardarelli; F. Cardillo; G. Carducci; I. Carli; T. Carli; G. Carlino; B. T. Carlson; L. Carminati; R. M. D. Carney; S. Caron; E. Carquin; S. Carrá; J. W. S. Carter; M. P. Casado; A. F. Casha; D. W. Casper; R. Castelijn; F. L. Castillo; V. Castillo Gimenez; N. F. Castro; A. Catinaccio; J. R. Catmore; A. Cattai; V. Cavaliere; E. Cavallaro; M. Cavalli-Sforza; V. Cavasinni; E. Celebi; F. Ceradini; L. Cerda Alberich; K. Cerny; A. S. Cerqueira; A. Cerri; L. Cerrito; F. Cerutti; A. Cervelli; S. A. Cetin; Z. Chadi; D. Chakraborty; W. S. Chan; W. Y. Chan; J. D. Chapman; B. Chargeishvili; D. G. Charlton; T. P. Charman; C. C. Chau; S. Che; S. Chekanov; S. V. Chekulaev; G. A. Chelkov; M. A. Chelstowska; B. Chen; C. Chen; C. H. Chen; H. Chen; J. Chen; S. Chen; S. J. Chen; X. Chen; Y-H. Chen; H. C. Cheng; H. J. Cheng; A. Cheplakov; E. Cheremushkina; R. Cherkaoui El Moursli; E. Cheu; K. Cheung; T. J. A. Chevalérias; L. Chevalier; V. Chiarella; G. Chiarelli; G. Chiodini; A. S. Chisholm; A. Chitan; I. Chiu; Y. H. Chiu; M. V. Chizhov; K. Choi; A. R. Chomont; S. Chouridou; Y. S. Chow; M. C. Chu; X. Chu; J. Chudoba; A. J. Chuinard; J. J. Chwastowski; L. Chytka; D. Cieri; K. M. Ciesla; D. Cinca; V. Cindro; I. A. Cioară; A. Ciocio; F. Cirotto; Z. H. Citron; M. Citterio; D. A. Ciubotaru; B. M. Ciungu; A. Clark; M. R. Clark; P. J. Clark; C. Clement; Y. Coadou; M. Cobal; A. Coccaro; J. Cochran; H. Cohen; A. E. C. Coimbra; L. Colasurdo; B. Cole; A. P. Colijn; J. Collot; P. Conde Muiño; S. H. Connell; I. A. Connelly; S. Constantinescu; F. Conventi; A. M. Cooper-Sarkar; F. Cormier; K. J. R. Cormier; L. D. Corpe; M. Corradi; E. E. Corrigan; F. Corriveau; A. Cortes-Gonzalez; M. J. Costa; F. Costanza; D. Costanzo; G. Cowan; J. W. Cowley; J. Crane; K. Cranmer; S. J. Crawley; R. A. Creager; S. Crépé-Renaudin; F. Crescioli; M. Cristinziani; V. Croft; G. Crosetti; A. Cueto; T. Cuhadar Donszelmann; A. R. Cukierman; W. R. Cunningham; S. Czekierda; P. Czodrowski; M. J. Da Cunha Sargedas De Sousa; J. V. Da Fonseca Pinto; C. Da Via; W. Dabrowski; F. Dachs; T. Dado; S. Dahbi; T. Dai; C. Dallapiccola; M. Dam; G. D'amen; V. D'Amico; J. Damp; J. R. Dandoy; M. F. Daneri; N. P. Dang; N. S. Dann; M. Danninger; V. Dao; G. Darbo; O. Dartsi; A. Dattagupta; T. Daubney; S. D'Auria; C. David; T. Davidek; D. R. Davis; I. Dawson; K. De; R. De Asmundis; M. De Beurs; S. De Castro; S. De Cecco; N. De Groot; P. de Jong; H. De la Torre; A. De Maria; D. De Pedis; A. De Salvo; U. De Sanctis; M. De Santis; A. De Santo; K. De Vasconcelos Corga; J. B. De Vivie De Regie; C. Debenedetti; D. V. Dedovich; A. M. Deiana; J. Del Peso; Y. Delabat Diaz; D. Delgove; F. Deliot; C. M. Delitzsch; M. Della Pietra; D. Della Volpe; A. Dell'Acqua; L. Dell'Asta; M. Delmastro; C. Delporte; P. A. Delsart; D. A. DeMarco; S. Demers; M. Demichev; G. Demontigny; S. P. Denisov; L. D'Eramo; D. Derendarz; J. E. Derkaoui; F. Derue; P. Dervan; K. Desch; C. Deterre; K. Dette; C. Deutsch; M. R. Devesa; P. O. Deviveiros; A. Dewhurst; F. A. Di Bello; A. Di Ciaccio; L. Di Ciaccio; W. K. Di Clemente; C. Di Donato; A. Di Girolamo; G. Di Gregorio; B. Di Micco; R. Di Nardo; K. F. Di Petrillo; R. Di Sipio; D. Di Valentino; C. Diaconu; F. A. Dias; T. Dias Do Vale; M. A. Diaz; J. Dickinson; E. B. Diehl; J. Dietrich; S. Díez Cornell; A. Dimitrievska; W. Ding; J. Dingfelder; F. Dittus; F. Djama; T. Djobava; J. I. Djuvsland; M. A. B. Do Vale; M. Dobre; D. Dodsworth; C. Doglioni; J. Dolejsi; Z. Dolezal; M. Donadelli; B. Dong; J. Donini; A. D'onofrio; M. D'Onofrio; J. Dopke; A. Doria; M. T. Dova; A. T. Doyle; E. Drechsler; E. Dreyer; T. Dreyer; A. S. Drobac; D. Du; Y. Duan; F. Dubinin; M. Dubovsky; A. Dubreuil; E. Duchovni; G. Duckeck; A. Ducourthial; O. A. Ducu; D. Duda; A. Dudarev; A. C. Dudder; E. M. Duffield; L. Duflot; M. Dührssen; C. Dülsen; M. Dumancic; A. E. Dumitriu; A. K. Duncan; M. Dunford; A. Duperrin; H. Duran Yildiz; M. Düren; A. Durglishvili; D. Duschinger; B. Dutta; D. Duvnjak; G. I. Dyckes; M. Dyndal; S. Dysch; B. S. Dziedzic; K. M. Ecker; R. C. Edgar; M. G. Eggleston; T. Eifert; G. Eigen; K. Einsweiler; T. Ekelof; H. El Jarrari; M. El Kacimi; R. El Kosseifi; V. Ellajosyula; M. Ellert; F. Ellinghaus; A. A. Elliot; N. Ellis; J. Elmsheuser; M. Elsing; D. Emeliyanov; A. Emerman; Y. Enari; M. B. Epland; J. Erdmann; A. Ereditato; M. Errenst; M. Escalier; C. Escobar; O. Estrada Pastor; E. Etzion; H. Evans; A. Ezhilov; F. Fabbri; L. Fabbri; V. Fabiani; G. Facini; R. M. Faisca Rodrigues Pereira; R. M. Fakhrutdinov; S. Falciano; P. J. Falke; S. Falke; J. Faltova; Y. Fang; G. Fanourakis; M. Fanti; M. Faraj; A. Farbin; A. Farilla; E. M. Farina; T. Farooque; S. Farrell; S. M. Farrington; P. Farthouat; F. Fassi; P. Fassnacht; D. Fassouliotis; M. Faucci Giannelli; W. J. Fawcett; L. Fayard; O. L. Fedin; W. Fedorko; A. Fehr; M. Feickert; L. Feligioni; A. Fell; C. Feng; M. Feng; M. J. Fenton; A. B. Fenyuk; S. W. Ferguson; J. Ferrando; A. Ferrante; A. Ferrari; P. Ferrari; R. Ferrari; D. E. Ferreira de Lima; A. Ferrer; D. Ferrere; C. Ferretti; F. Fiedler; A. Filipčič; F. Filthaut; K. D. Finelli; M. C. N. Fiolhais; L. Fiorini; F. Fischer; W. C. Fisher; I. Fleck; P. Fleischmann; R. R. M. Fletcher; T. Flick; B. M. Flierl; L. Flores; L. R. Flores Castillo; F. M. Follega; N. Fomin; J. H. Foo; G. T. Forcolin; A. Formica; F. A. Förster; A. C. Forti; A. G. Foster; M. G. Foti; D. Fournier; H. Fox; P. Francavilla; S. Francescato; M. Franchini; S. Franchino; D. Francis; L. Franconi; M. Franklin; A. N. Fray; P. M. Freeman; B. Freund; W. S. Freund; E. M. Freundlich; D. C. Frizzell; D. Froidevaux; J. A. Frost; C. Fukunaga; E. Fullana Torregrosa; E. Fumagalli; T. Fusayasu; J. Fuster; A. Gabrielli; S. Gadatsch; P. Gadow; G. Gagliardi; L. G. Gagnon; C. Galea; B. Galhardo; G. E. Gallardo; E. J. Gallas; B. J. Gallop; G. Galster; R. Gamboa Goni; K. K. Gan; S. Ganguly; J. Gao; Y. Gao; Y. S. Gao; C. García; J. E. García Navarro; J. A. García Pascual; C. Garcia-Argos; M. Garcia-Sciveres; R. W. Gardner; N. Garelli; S. Gargiulo; C. A. Garner; V. Garonne; S. J. Gasiorowski; P. Gaspar; A. Gaudiello; G. Gaudio; I. L. Gavrilenko; A. Gavrilyuk; C. Gay; G. Gaycken; E. N. Gazis; A. A. Geanta; C. M. Gee; C. N. P. Gee; J. Geisen; M. Geisen; C. Gemme; M. H. Genest; C. Geng; S. Gentile; S. George; T. Geralis; L. O. Gerlach; P. Gessinger-Befurt; G. Gessner; S. Ghasemi; M. Ghasemi Bostanabad; M. Ghneimat; A. Ghosh; B. Giacobbe; S. Giagu; N. Giangiacomi; P. Giannetti; A. Giannini; G. Giannini; S. M. Gibson; M. Gignac; D. Gillberg; G. Gilles; D. M. Gingrich; M. P. Giordani; F. M. Giorgi; P. F. Giraud; G. Giugliarelli; D. Giugni; F. Giuli; S. Gkaitatzis; I. Gkialas; E. L. Gkougkousis; P. Gkountoumis; L. K. Gladilin; C. Glasman; J. Glatzer; P. C. F. Glaysher; A. Glazov; G. R. Gledhill; M. Goblirsch-Kolb; D. Godin; S. Goldfarb; T. Golling; D. Golubkov; A. Gomes; R. Goncalves Gama; R. Gonçalo; G. Gonella; L. Gonella; A. Gongadze; F. Gonnella; J. L. Gonski; S. González de la Hoz; S. Gonzalez-Sevilla; G. R. Gonzalvo Rodriguez; L. Goossens; N. A. Gorasia; P. A. Gorbounov; H. A. Gordon; B. Gorini; E. Gorini; A. Gorišek; A. T. Goshaw; M. I. Gostkin; C. A. Gottardo; M. Gouighri; D. Goujdami; A. G. Goussiou; N. Govender; C. Goy; E. Gozani; I. Grabowska-Bold; E. C. Graham; J. Gramling; E. Gramstad; S. Grancagnolo; M. Grandi; V. Gratchev; P. M. Gravila; F. G. Gravili; C. Gray; H. M. Gray; C. Grefe; K. Gregersen; I. M. Gregor; P. Grenier; K. Grevtsov; C. Grieco; N. A. Grieser; A. A. Grillo; K. Grimm; S. Grinstein; J.-F. Grivaz; S. Groh; E. Gross; J. Grosse-Knetter; Z. J. Grout; C. Grud; A. Grummer; L. Guan; W. Guan; C. Gubbels; J. Guenther; A. Guerguichon; J. G. R. Guerrero Rojas; F. Guescini; D. Guest; R. Gugel; T. Guillemin; S. Guindon; U. Gul; J. Guo; W. Guo; Y. Guo; Z. Guo; R. Gupta; S. Gurbuz; G. Gustavino and M. 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  Data: Measurement of the $$t\bar{t}$$ tt¯ production cross-section and lepton differential distributions in $$e\mu $$ eμ dilepton events from pp collisions at $$\sqrt{s}=13\,\text {TeV}$$ s=13TeV with the ATLAS detector
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Bakalis</searchLink><br /><searchLink fieldCode="AR" term="%22O%2E+K%2E+Baker%22">O. K. Baker</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+J%2E+Bakker%22">P. J. Bakker</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Bakshi+Gupta%22">D. Bakshi Gupta</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Balaji%22">S. Balaji</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+M%2E+Baldin%22">E. M. Baldin</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Balek%22">P. Balek</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Balli%22">F. Balli</searchLink><br /><searchLink fieldCode="AR" term="%22W%2E+K%2E+Balunas%22">W. K. Balunas</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Balz%22">J. Balz</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Banas%22">E. Banas</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Bandyopadhyay%22">A. Bandyopadhyay</searchLink><br /><searchLink fieldCode="AR" term="%22Sw%2E+Banerjee%22">Sw. Banerjee</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+A%2E+E%2E+Bannoura%22">A. A. E. Bannoura</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Barak%22">L. Barak</searchLink><br /><searchLink fieldCode="AR" term="%22W%2E+M%2E+Barbe%22">W. M. Barbe</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+L%2E+Barberio%22">E. L. Barberio</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Barberis%22">D. Barberis</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Barbero%22">M. Barbero</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Barbour%22">G. Barbour</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Barillari%22">T. Barillari</searchLink><br /><searchLink fieldCode="AR" term="%22M-S%2E+Barisits%22">M-S. Barisits</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Barkeloo%22">J. Barkeloo</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Barklow%22">T. Barklow</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Barnea%22">R. Barnea</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+L%2E+Barnes%22">S. L. Barnes</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+M%2E+Barnett%22">B. M. Barnett</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+M%2E+Barnett%22">R. M. Barnett</searchLink><br /><searchLink fieldCode="AR" term="%22Z%2E+Barnovska-Blenessy%22">Z. Barnovska-Blenessy</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Baroncelli%22">A. Baroncelli</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Barone%22">G. Barone</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+J%2E+Barr%22">A. J. Barr</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Barranco+Navarro%22">L. Barranco Navarro</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Barreiro%22">F. Barreiro</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Barreiro+Guimarães+da+Costa%22">J. Barreiro Guimarães da Costa</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Barsov%22">S. Barsov</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Bartoldus%22">R. Bartoldus</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Bartolini%22">G. Bartolini</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+E%2E+Barton%22">A. E. Barton</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Bartos%22">P. Bartos</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Basalaev%22">A. Basalaev</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Basan%22">A. Basan</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Bassalat%22">A. Bassalat</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+J%2E+Basso%22">M. J. Basso</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+L%2E+Bates%22">R. L. Bates</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Batlamous%22">S. Batlamous</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+R%2E+Batley%22">J. R. Batley</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Batool%22">B. Batool</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Battaglia%22">M. Battaglia</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Bauce%22">M. Bauce</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Bauer%22">F. Bauer</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+T%2E+Bauer%22">K. T. Bauer</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+S%2E+Bawa%22">H. S. Bawa</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+B%2E+Beacham%22">J. B. Beacham</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Beau%22">T. Beau</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+H%2E+Beauchemin%22">P. H. Beauchemin</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Becherer%22">F. Becherer</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Bechtle%22">P. Bechtle</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+C%2E+Beck%22">H. C. Beck</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+P%2E+Beck%22">H. P. Beck</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Becker%22">K. Becker</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Becker%22">M. Becker</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Becot%22">C. Becot</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Beddall%22">A. Beddall</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+J%2E+Beddall%22">A. J. Beddall</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+A%2E+Bednyakov%22">V. A. Bednyakov</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Bedognetti%22">M. Bedognetti</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+P%2E+Bee%22">C. P. Bee</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+A%2E+Beermann%22">T. A. Beermann</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Begalli%22">M. Begalli</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Begel%22">M. Begel</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Behera%22">A. Behera</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+K%2E+Behr%22">J. K. Behr</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Beisiegel%22">F. Beisiegel</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+S%2E+Bell%22">A. S. Bell</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Bella%22">G. Bella</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Bellagamba%22">L. Bellagamba</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Bellerive%22">A. Bellerive</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Bellos%22">P. Bellos</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Beloborodov%22">K. Beloborodov</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Belotskiy%22">K. Belotskiy</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+L%2E+Belyaev%22">N. L. Belyaev</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Benchekroun%22">D. Benchekroun</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+Benekos%22">N. Benekos</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+Benhammou%22">Y. Benhammou</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+P%2E+Benjamin%22">D. P. Benjamin</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Benoit%22">M. Benoit</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+R%2E+Bensinger%22">J. R. Bensinger</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Bentvelsen%22">S. Bentvelsen</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Beresford%22">L. Beresford</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Beretta%22">M. Beretta</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Berge%22">D. Berge</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Bergeaas+Kuutmann%22">E. Bergeaas Kuutmann</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+Berger%22">N. Berger</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Bergmann%22">B. Bergmann</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+J%2E+Bergsten%22">L. J. Bergsten</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Beringer%22">J. Beringer</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Berlendis%22">S. Berlendis</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Bernardi%22">G. Bernardi</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Bernius%22">C. Bernius</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+U%2E+Bernlochner%22">F. U. Bernlochner</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Berry%22">T. Berry</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Berta%22">P. Berta</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Bertella%22">C. Bertella</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+A%2E+Bertram%22">I. A. Bertram</searchLink><br /><searchLink fieldCode="AR" term="%22O%2E+Bessidskaia+Bylund%22">O. Bessidskaia Bylund</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+Besson%22">N. Besson</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Bethani%22">A. Bethani</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Bethke%22">S. Bethke</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Betti%22">A. Betti</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+J%2E+Bevan%22">A. J. Bevan</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Beyer%22">J. Beyer</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+S%2E+Bhattacharya%22">D. S. Bhattacharya</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Bhattarai%22">P. Bhattarai</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Bi%22">R. Bi</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+M%2E+Bianchi%22">R. M. Bianchi</searchLink><br /><searchLink fieldCode="AR" term="%22O%2E+Biebel%22">O. Biebel</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Biedermann%22">D. Biedermann</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Bielski%22">R. Bielski</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Bierwagen%22">K. Bierwagen</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+V%2E+Biesuz%22">N. V. Biesuz</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Biglietti%22">M. Biglietti</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+R%2E+V%2E+Billoud%22">T. R. V. Billoud</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Bindi%22">M. Bindi</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Bingul%22">A. Bingul</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Bini%22">C. Bini</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Biondi%22">S. Biondi</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Birman%22">M. Birman</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Bisanz%22">T. Bisanz</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+P%2E+Biswal%22">J. P. Biswal</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Biswas%22">D. Biswas</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Bitadze%22">A. Bitadze</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Bittrich%22">C. Bittrich</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Bjørke%22">K. Bjørke</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+M%2E+Black%22">K. M. Black</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Blazek%22">T. Blazek</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+Bloch%22">I. Bloch</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Blocker%22">C. Blocker</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Blue%22">A. Blue</searchLink><br /><searchLink fieldCode="AR" term="%22U%2E+Blumenschein%22">U. Blumenschein</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+J%2E+Bobbink%22">G. J. Bobbink</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+S%2E+Bobrovnikov%22">V. S. Bobrovnikov</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+S%2E+Bocchetta%22">S. S. Bocchetta</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Bocci%22">A. Bocci</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Boerner%22">D. Boerner</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Bogavac%22">D. Bogavac</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+G%2E+Bogdanchikov%22">A. G. Bogdanchikov</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Bohm%22">C. Bohm</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+Boisvert%22">V. Boisvert</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Bokan%22">P. Bokan</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Bold%22">T. Bold</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+S%2E+Boldyrev%22">A. S. Boldyrev</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+E%2E+Bolz%22">A. E. Bolz</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Bomben%22">M. Bomben</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Bona%22">M. Bona</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+S%2E+Bonilla%22">J. S. Bonilla</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Boonekamp%22">M. Boonekamp</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+D%2E+Booth%22">C. D. Booth</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+M%2E+Borecka-Bielska%22">H. M. Borecka-Bielska</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Borisov%22">A. Borisov</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Borissov%22">G. Borissov</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Bortfeldt%22">J. Bortfeldt</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Bortoletto%22">D. Bortoletto</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Boscherini%22">D. Boscherini</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Bosman%22">M. Bosman</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+D%2E+Bossio+Sola%22">J. D. Bossio Sola</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Bouaouda%22">K. Bouaouda</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Boudreau%22">J. Boudreau</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+V%2E+Bouhova-Thacker%22">E. V. Bouhova-Thacker</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Boumediene%22">D. Boumediene</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+K%2E+Boutle%22">S. K. Boutle</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Boveia%22">A. Boveia</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Boyd%22">J. Boyd</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Boye%22">D. Boye</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+R%2E+Boyko%22">I. R. Boyko</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+J%2E+Bozson%22">A. J. Bozson</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Bracinik%22">J. Bracinik</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+Brahimi%22">N. Brahimi</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Brandt%22">G. Brandt</searchLink><br /><searchLink fieldCode="AR" term="%22O%2E+Brandt%22">O. Brandt</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Braren%22">F. Braren</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Brau%22">B. Brau</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+E%2E+Brau%22">J. E. Brau</searchLink><br /><searchLink fieldCode="AR" term="%22W%2E+D%2E+Breaden+Madden%22">W. D. Breaden Madden</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Brendlinger%22">K. Brendlinger</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Brenner%22">L. Brenner</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Brenner%22">R. Brenner</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Bressler%22">S. Bressler</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Brickwedde%22">B. Brickwedde</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+L%2E+Briglin%22">D. L. Briglin</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Britton%22">D. Britton</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Britzger%22">D. Britzger</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+Brock%22">I. Brock</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Brock%22">R. Brock</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Brooijmans%22">G. Brooijmans</searchLink><br /><searchLink fieldCode="AR" term="%22W%2E+K%2E+Brooks%22">W. K. Brooks</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Brost%22">E. Brost</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+H%2E+Broughton%22">J. H. Broughton</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+A%2E+Bruckman+de+Renstrom%22">P. A. Bruckman de Renstrom</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Bruncko%22">D. Bruncko</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Bruni%22">A. Bruni</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Bruni%22">G. Bruni</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+S%2E+Bruni%22">L. S. Bruni</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Bruno%22">S. Bruno</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Bruschi%22">M. Bruschi</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+Bruscino%22">N. Bruscino</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Bryant%22">P. Bryant</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Bryngemark%22">L. Bryngemark</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Buanes%22">T. Buanes</searchLink><br /><searchLink fieldCode="AR" term="%22Q%2E+Buat%22">Q. Buat</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Buchholz%22">P. Buchholz</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+G%2E+Buckley%22">A. G. Buckley</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+A%2E+Budagov%22">I. A. Budagov</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+K%2E+Bugge%22">M. K. Bugge</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Bührer%22">F. Bührer</searchLink><br /><searchLink fieldCode="AR" term="%22O%2E+Bulekov%22">O. Bulekov</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+J%2E+Burch%22">T. J. Burch</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Burdin%22">S. Burdin</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+D%2E+Burgard%22">C. D. Burgard</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+M%2E+Burger%22">A. M. Burger</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Burghgrave%22">B. Burghgrave</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+T%2E+P%2E+Burr%22">J. T. P. Burr</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+D%2E+Burton%22">C. D. Burton</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+C%2E+Burzynski%22">J. C. Burzynski</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+Büscher%22">V. Büscher</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Buschmann%22">E. Buschmann</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+J%2E+Bussey%22">P. J. Bussey</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+M%2E+Butler%22">J. M. Butler</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+M%2E+Buttar%22">C. M. Buttar</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+M%2E+Butterworth%22">J. M. Butterworth</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Butti%22">P. Butti</searchLink><br /><searchLink fieldCode="AR" term="%22W%2E+Buttinger%22">W. Buttinger</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+J%2E+Buxo+Vazquez%22">C. J. Buxo Vazquez</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Buzatu%22">A. Buzatu</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+R%2E+Buzykaev%22">A. R. Buzykaev</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Cabras%22">G. Cabras</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Cabrera+Urbán%22">S. Cabrera Urbán</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Caforio%22">D. Caforio</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+Cai%22">H. Cai</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+M%2E+M%2E+Cairo%22">V. M. M. Cairo</searchLink><br /><searchLink fieldCode="AR" term="%22O%2E+Cakir%22">O. Cakir</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+Calace%22">N. Calace</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Calafiura%22">P. Calafiura</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Calandri%22">A. Calandri</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Calderini%22">G. Calderini</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Calfayan%22">P. Calfayan</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Callea%22">G. Callea</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+P%2E+Caloba%22">L. P. Caloba</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Caltabiano%22">A. Caltabiano</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Calvente+Lopez%22">S. Calvente Lopez</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Calvet%22">D. Calvet</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Calvet%22">S. Calvet</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+P%2E+Calvet%22">T. P. Calvet</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Calvetti%22">M. Calvetti</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Camacho+Toro%22">R. Camacho Toro</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Camarda%22">S. Camarda</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Camarero+Munoz%22">D. Camarero Munoz</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Camarri%22">P. Camarri</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Cameron%22">D. Cameron</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Caminal+Armadans%22">R. Caminal Armadans</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Camincher%22">C. Camincher</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Campana%22">S. Campana</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Campanelli%22">M. Campanelli</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Camplani%22">A. Camplani</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Campoverde%22">A. Campoverde</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+Canale%22">V. Canale</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Canesse%22">A. Canesse</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Cano+Bret%22">M. Cano Bret</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Cantero%22">J. Cantero</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Cao%22">T. Cao</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+Cao%22">Y. Cao</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+D%2E+M%2E+Capeans+Garrido%22">M. D. M. Capeans Garrido</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Capua%22">M. Capua</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Cardarelli%22">R. Cardarelli</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Cardillo%22">F. Cardillo</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Carducci%22">G. Carducci</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+Carli%22">I. Carli</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Carli%22">T. Carli</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Carlino%22">G. Carlino</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+T%2E+Carlson%22">B. T. Carlson</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Carminati%22">L. Carminati</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+M%2E+D%2E+Carney%22">R. M. D. Carney</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Caron%22">S. Caron</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Carquin%22">E. Carquin</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Carrá%22">S. Carrá</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+W%2E+S%2E+Carter%22">J. W. S. Carter</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+P%2E+Casado%22">M. P. Casado</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+F%2E+Casha%22">A. F. Casha</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+W%2E+Casper%22">D. W. Casper</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Castelijn%22">R. Castelijn</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+L%2E+Castillo%22">F. L. Castillo</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+Castillo+Gimenez%22">V. Castillo Gimenez</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+F%2E+Castro%22">N. F. Castro</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Catinaccio%22">A. Catinaccio</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+R%2E+Catmore%22">J. R. Catmore</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Cattai%22">A. Cattai</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+Cavaliere%22">V. Cavaliere</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Cavallaro%22">E. Cavallaro</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Cavalli-Sforza%22">M. Cavalli-Sforza</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+Cavasinni%22">V. Cavasinni</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Celebi%22">E. Celebi</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Ceradini%22">F. Ceradini</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Cerda+Alberich%22">L. Cerda Alberich</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Cerny%22">K. Cerny</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+S%2E+Cerqueira%22">A. S. Cerqueira</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Cerri%22">A. Cerri</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Cerrito%22">L. Cerrito</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Cerutti%22">F. Cerutti</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Cervelli%22">A. Cervelli</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+A%2E+Cetin%22">S. A. Cetin</searchLink><br /><searchLink fieldCode="AR" term="%22Z%2E+Chadi%22">Z. Chadi</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Chakraborty%22">D. Chakraborty</searchLink><br /><searchLink fieldCode="AR" term="%22W%2E+S%2E+Chan%22">W. S. Chan</searchLink><br /><searchLink fieldCode="AR" term="%22W%2E+Y%2E+Chan%22">W. Y. Chan</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+D%2E+Chapman%22">J. D. Chapman</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Chargeishvili%22">B. Chargeishvili</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+G%2E+Charlton%22">D. G. Charlton</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+P%2E+Charman%22">T. P. Charman</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+C%2E+Chau%22">C. C. Chau</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Che%22">S. Che</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Chekanov%22">S. Chekanov</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+V%2E+Chekulaev%22">S. V. Chekulaev</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+A%2E+Chelkov%22">G. A. Chelkov</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+A%2E+Chelstowska%22">M. A. Chelstowska</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Chen%22">B. Chen</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Chen%22">C. Chen</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+H%2E+Chen%22">C. H. Chen</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+Chen%22">H. Chen</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Chen%22">J. Chen</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Chen%22">S. Chen</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+J%2E+Chen%22">S. J. Chen</searchLink><br /><searchLink fieldCode="AR" term="%22X%2E+Chen%22">X. Chen</searchLink><br /><searchLink fieldCode="AR" term="%22Y-H%2E+Chen%22">Y-H. Chen</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+C%2E+Cheng%22">H. C. Cheng</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+J%2E+Cheng%22">H. J. Cheng</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Cheplakov%22">A. Cheplakov</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Cheremushkina%22">E. Cheremushkina</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Cherkaoui+El+Moursli%22">R. Cherkaoui El Moursli</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Cheu%22">E. Cheu</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Cheung%22">K. Cheung</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+J%2E+A%2E+Chevalérias%22">T. J. A. Chevalérias</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Chevalier%22">L. Chevalier</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+Chiarella%22">V. Chiarella</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Chiarelli%22">G. Chiarelli</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Chiodini%22">G. Chiodini</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+S%2E+Chisholm%22">A. S. Chisholm</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Chitan%22">A. Chitan</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+Chiu%22">I. Chiu</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+H%2E+Chiu%22">Y. H. Chiu</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+V%2E+Chizhov%22">M. V. Chizhov</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Choi%22">K. Choi</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+R%2E+Chomont%22">A. R. Chomont</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Chouridou%22">S. Chouridou</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+S%2E+Chow%22">Y. S. Chow</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+C%2E+Chu%22">M. C. Chu</searchLink><br /><searchLink fieldCode="AR" term="%22X%2E+Chu%22">X. Chu</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Chudoba%22">J. Chudoba</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+J%2E+Chuinard%22">A. J. Chuinard</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+J%2E+Chwastowski%22">J. J. Chwastowski</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Chytka%22">L. Chytka</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Cieri%22">D. Cieri</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+M%2E+Ciesla%22">K. M. Ciesla</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Cinca%22">D. Cinca</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+Cindro%22">V. Cindro</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+A%2E+Cioară%22">I. A. Cioară</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Ciocio%22">A. Ciocio</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Cirotto%22">F. Cirotto</searchLink><br /><searchLink fieldCode="AR" term="%22Z%2E+H%2E+Citron%22">Z. H. Citron</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Citterio%22">M. Citterio</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+A%2E+Ciubotaru%22">D. A. Ciubotaru</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+M%2E+Ciungu%22">B. M. Ciungu</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Clark%22">A. Clark</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+R%2E+Clark%22">M. R. Clark</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+J%2E+Clark%22">P. J. Clark</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Clement%22">C. Clement</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+Coadou%22">Y. Coadou</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Cobal%22">M. Cobal</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Coccaro%22">A. Coccaro</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Cochran%22">J. Cochran</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+Cohen%22">H. Cohen</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+E%2E+C%2E+Coimbra%22">A. E. C. Coimbra</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Colasurdo%22">L. Colasurdo</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Cole%22">B. Cole</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+P%2E+Colijn%22">A. P. Colijn</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Collot%22">J. Collot</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Conde+Muiño%22">P. Conde Muiño</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+H%2E+Connell%22">S. H. Connell</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+A%2E+Connelly%22">I. A. Connelly</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Constantinescu%22">S. Constantinescu</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Conventi%22">F. Conventi</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+M%2E+Cooper-Sarkar%22">A. M. Cooper-Sarkar</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Cormier%22">F. Cormier</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+J%2E+R%2E+Cormier%22">K. J. R. Cormier</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+D%2E+Corpe%22">L. D. Corpe</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Corradi%22">M. Corradi</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+E%2E+Corrigan%22">E. E. Corrigan</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Corriveau%22">F. Corriveau</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Cortes-Gonzalez%22">A. Cortes-Gonzalez</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+J%2E+Costa%22">M. J. Costa</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Costanza%22">F. Costanza</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Costanzo%22">D. Costanzo</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Cowan%22">G. Cowan</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+W%2E+Cowley%22">J. W. Cowley</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Crane%22">J. Crane</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Cranmer%22">K. Cranmer</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+J%2E+Crawley%22">S. J. Crawley</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+A%2E+Creager%22">R. A. Creager</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Crépé-Renaudin%22">S. Crépé-Renaudin</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Crescioli%22">F. Crescioli</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Cristinziani%22">M. Cristinziani</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+Croft%22">V. Croft</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Crosetti%22">G. Crosetti</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Cueto%22">A. Cueto</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Cuhadar+Donszelmann%22">T. Cuhadar Donszelmann</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+R%2E+Cukierman%22">A. R. Cukierman</searchLink><br /><searchLink fieldCode="AR" term="%22W%2E+R%2E+Cunningham%22">W. R. Cunningham</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Czekierda%22">S. Czekierda</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Czodrowski%22">P. Czodrowski</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+J%2E+Da+Cunha+Sargedas+De+Sousa%22">M. J. Da Cunha Sargedas De Sousa</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+V%2E+Da+Fonseca+Pinto%22">J. V. Da Fonseca Pinto</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Da+Via%22">C. Da Via</searchLink><br /><searchLink fieldCode="AR" term="%22W%2E+Dabrowski%22">W. Dabrowski</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Dachs%22">F. Dachs</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Dado%22">T. Dado</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Dahbi%22">S. Dahbi</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Dai%22">T. Dai</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Dallapiccola%22">C. Dallapiccola</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Dam%22">M. Dam</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+D%27amen%22">G. D’amen</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+D%27Amico%22">V. D’Amico</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Damp%22">J. Damp</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+R%2E+Dandoy%22">J. R. Dandoy</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+F%2E+Daneri%22">M. F. Daneri</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+P%2E+Dang%22">N. P. Dang</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+S%2E+Dann%22">N. S. Dann</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Danninger%22">M. Danninger</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+Dao%22">V. Dao</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Darbo%22">G. Darbo</searchLink><br /><searchLink fieldCode="AR" term="%22O%2E+Dartsi%22">O. Dartsi</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Dattagupta%22">A. Dattagupta</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Daubney%22">T. Daubney</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+D%27Auria%22">S. D’Auria</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+David%22">C. David</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Davidek%22">T. Davidek</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+R%2E+Davis%22">D. R. Davis</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+Dawson%22">I. Dawson</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+De%22">K. De</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+De+Asmundis%22">R. De Asmundis</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+De+Beurs%22">M. De Beurs</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+De+Castro%22">S. De Castro</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+De+Cecco%22">S. De Cecco</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+De+Groot%22">N. De Groot</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+de+Jong%22">P. de Jong</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+De+la+Torre%22">H. De la Torre</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+De+Maria%22">A. De Maria</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+De+Pedis%22">D. De Pedis</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+De+Salvo%22">A. De Salvo</searchLink><br /><searchLink fieldCode="AR" term="%22U%2E+De+Sanctis%22">U. De Sanctis</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+De+Santis%22">M. De Santis</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+De+Santo%22">A. De Santo</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+De+Vasconcelos+Corga%22">K. De Vasconcelos Corga</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+B%2E+De+Vivie+De+Regie%22">J. B. De Vivie De Regie</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Debenedetti%22">C. Debenedetti</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+V%2E+Dedovich%22">D. V. Dedovich</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+M%2E+Deiana%22">A. M. Deiana</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Del+Peso%22">J. Del Peso</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+Delabat+Diaz%22">Y. Delabat Diaz</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Delgove%22">D. Delgove</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Deliot%22">F. Deliot</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+M%2E+Delitzsch%22">C. M. Delitzsch</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Della+Pietra%22">M. Della Pietra</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Della+Volpe%22">D. Della Volpe</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Dell%27Acqua%22">A. Dell’Acqua</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Dell%27Asta%22">L. Dell’Asta</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Delmastro%22">M. Delmastro</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Delporte%22">C. Delporte</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+A%2E+Delsart%22">P. A. Delsart</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+A%2E+DeMarco%22">D. A. DeMarco</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Demers%22">S. Demers</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Demichev%22">M. Demichev</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Demontigny%22">G. Demontigny</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+P%2E+Denisov%22">S. P. Denisov</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+D%27Eramo%22">L. D’Eramo</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Derendarz%22">D. Derendarz</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+E%2E+Derkaoui%22">J. E. Derkaoui</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Derue%22">F. Derue</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Dervan%22">P. Dervan</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Desch%22">K. Desch</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Deterre%22">C. Deterre</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Dette%22">K. Dette</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Deutsch%22">C. Deutsch</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+R%2E+Devesa%22">M. R. Devesa</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+O%2E+Deviveiros%22">P. O. Deviveiros</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Dewhurst%22">A. Dewhurst</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+A%2E+Di+Bello%22">F. A. Di Bello</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Di+Ciaccio%22">A. Di Ciaccio</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Di+Ciaccio%22">L. Di Ciaccio</searchLink><br /><searchLink fieldCode="AR" term="%22W%2E+K%2E+Di+Clemente%22">W. K. Di Clemente</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Di+Donato%22">C. Di Donato</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Di+Girolamo%22">A. Di Girolamo</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Di+Gregorio%22">G. Di Gregorio</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Di+Micco%22">B. Di Micco</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Di+Nardo%22">R. Di Nardo</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+F%2E+Di+Petrillo%22">K. F. Di Petrillo</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Di+Sipio%22">R. Di Sipio</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Di+Valentino%22">D. Di Valentino</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Diaconu%22">C. Diaconu</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+A%2E+Dias%22">F. A. Dias</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Dias+Do+Vale%22">T. Dias Do Vale</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+A%2E+Diaz%22">M. A. Diaz</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Dickinson%22">J. Dickinson</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+B%2E+Diehl%22">E. B. Diehl</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Dietrich%22">J. Dietrich</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Díez+Cornell%22">S. Díez Cornell</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Dimitrievska%22">A. Dimitrievska</searchLink><br /><searchLink fieldCode="AR" term="%22W%2E+Ding%22">W. Ding</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Dingfelder%22">J. Dingfelder</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Dittus%22">F. Dittus</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Djama%22">F. Djama</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Djobava%22">T. Djobava</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+I%2E+Djuvsland%22">J. I. Djuvsland</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+A%2E+B%2E+Do+Vale%22">M. A. B. Do Vale</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Dobre%22">M. Dobre</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Dodsworth%22">D. Dodsworth</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Doglioni%22">C. Doglioni</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Dolejsi%22">J. Dolejsi</searchLink><br /><searchLink fieldCode="AR" term="%22Z%2E+Dolezal%22">Z. Dolezal</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Donadelli%22">M. Donadelli</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Dong%22">B. Dong</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Donini%22">J. Donini</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+D%27onofrio%22">A. D’onofrio</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+D%27Onofrio%22">M. D’Onofrio</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Dopke%22">J. Dopke</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Doria%22">A. Doria</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+T%2E+Dova%22">M. T. Dova</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+T%2E+Doyle%22">A. T. Doyle</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Drechsler%22">E. Drechsler</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Dreyer%22">E. Dreyer</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Dreyer%22">T. Dreyer</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+S%2E+Drobac%22">A. S. Drobac</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Du%22">D. Du</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+Duan%22">Y. Duan</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Dubinin%22">F. Dubinin</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Dubovsky%22">M. Dubovsky</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Dubreuil%22">A. Dubreuil</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Duchovni%22">E. Duchovni</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Duckeck%22">G. Duckeck</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Ducourthial%22">A. Ducourthial</searchLink><br /><searchLink fieldCode="AR" term="%22O%2E+A%2E+Ducu%22">O. A. Ducu</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Duda%22">D. Duda</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Dudarev%22">A. Dudarev</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+C%2E+Dudder%22">A. C. Dudder</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+M%2E+Duffield%22">E. M. Duffield</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Duflot%22">L. Duflot</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Dührssen%22">M. Dührssen</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Dülsen%22">C. Dülsen</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Dumancic%22">M. Dumancic</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+E%2E+Dumitriu%22">A. E. Dumitriu</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+K%2E+Duncan%22">A. K. Duncan</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Dunford%22">M. Dunford</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Duperrin%22">A. Duperrin</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+Duran+Yildiz%22">H. Duran Yildiz</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Düren%22">M. Düren</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Durglishvili%22">A. Durglishvili</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Duschinger%22">D. Duschinger</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Dutta%22">B. Dutta</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Duvnjak%22">D. Duvnjak</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+I%2E+Dyckes%22">G. I. Dyckes</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Dyndal%22">M. Dyndal</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Dysch%22">S. Dysch</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+S%2E+Dziedzic%22">B. S. Dziedzic</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+M%2E+Ecker%22">K. M. Ecker</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+C%2E+Edgar%22">R. C. Edgar</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+G%2E+Eggleston%22">M. G. Eggleston</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Eifert%22">T. Eifert</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Eigen%22">G. Eigen</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Einsweiler%22">K. Einsweiler</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Ekelof%22">T. Ekelof</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+El+Jarrari%22">H. El Jarrari</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+El+Kacimi%22">M. El Kacimi</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+El+Kosseifi%22">R. El Kosseifi</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+Ellajosyula%22">V. Ellajosyula</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Ellert%22">M. Ellert</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Ellinghaus%22">F. Ellinghaus</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+A%2E+Elliot%22">A. A. Elliot</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+Ellis%22">N. Ellis</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Elmsheuser%22">J. Elmsheuser</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Elsing%22">M. Elsing</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Emeliyanov%22">D. Emeliyanov</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Emerman%22">A. Emerman</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+Enari%22">Y. Enari</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+B%2E+Epland%22">M. B. Epland</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Erdmann%22">J. Erdmann</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Ereditato%22">A. Ereditato</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Errenst%22">M. Errenst</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Escalier%22">M. Escalier</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Escobar%22">C. Escobar</searchLink><br /><searchLink fieldCode="AR" term="%22O%2E+Estrada+Pastor%22">O. Estrada Pastor</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Etzion%22">E. Etzion</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+Evans%22">H. Evans</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Ezhilov%22">A. Ezhilov</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Fabbri%22">F. Fabbri</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Fabbri%22">L. Fabbri</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+Fabiani%22">V. Fabiani</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Facini%22">G. Facini</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+M%2E+Faisca+Rodrigues+Pereira%22">R. M. Faisca Rodrigues Pereira</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+M%2E+Fakhrutdinov%22">R. M. Fakhrutdinov</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Falciano%22">S. Falciano</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+J%2E+Falke%22">P. J. Falke</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Falke%22">S. Falke</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Faltova%22">J. Faltova</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+Fang%22">Y. Fang</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Fanourakis%22">G. Fanourakis</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Fanti%22">M. Fanti</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Faraj%22">M. Faraj</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Farbin%22">A. Farbin</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Farilla%22">A. Farilla</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+M%2E+Farina%22">E. M. Farina</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Farooque%22">T. Farooque</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Farrell%22">S. Farrell</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+M%2E+Farrington%22">S. M. Farrington</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Farthouat%22">P. Farthouat</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Fassi%22">F. Fassi</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Fassnacht%22">P. Fassnacht</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Fassouliotis%22">D. Fassouliotis</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Faucci+Giannelli%22">M. Faucci Giannelli</searchLink><br /><searchLink fieldCode="AR" term="%22W%2E+J%2E+Fawcett%22">W. J. Fawcett</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Fayard%22">L. Fayard</searchLink><br /><searchLink fieldCode="AR" term="%22O%2E+L%2E+Fedin%22">O. L. Fedin</searchLink><br /><searchLink fieldCode="AR" term="%22W%2E+Fedorko%22">W. Fedorko</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Fehr%22">A. Fehr</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Feickert%22">M. Feickert</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Feligioni%22">L. Feligioni</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Fell%22">A. Fell</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Feng%22">C. Feng</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Feng%22">M. Feng</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+J%2E+Fenton%22">M. J. Fenton</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+B%2E+Fenyuk%22">A. B. Fenyuk</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+W%2E+Ferguson%22">S. W. Ferguson</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Ferrando%22">J. Ferrando</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Ferrante%22">A. Ferrante</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Ferrari%22">A. Ferrari</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Ferrari%22">P. Ferrari</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Ferrari%22">R. Ferrari</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+E%2E+Ferreira+de+Lima%22">D. E. Ferreira de Lima</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Ferrer%22">A. Ferrer</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Ferrere%22">D. Ferrere</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Ferretti%22">C. Ferretti</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Fiedler%22">F. Fiedler</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Filipčič%22">A. Filipčič</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Filthaut%22">F. Filthaut</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+D%2E+Finelli%22">K. D. Finelli</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+C%2E+N%2E+Fiolhais%22">M. C. N. Fiolhais</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Fiorini%22">L. Fiorini</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Fischer%22">F. Fischer</searchLink><br /><searchLink fieldCode="AR" term="%22W%2E+C%2E+Fisher%22">W. C. Fisher</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+Fleck%22">I. Fleck</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Fleischmann%22">P. Fleischmann</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+R%2E+M%2E+Fletcher%22">R. R. M. Fletcher</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Flick%22">T. Flick</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+M%2E+Flierl%22">B. M. Flierl</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Flores%22">L. Flores</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+R%2E+Flores+Castillo%22">L. R. Flores Castillo</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+M%2E+Follega%22">F. M. Follega</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+Fomin%22">N. Fomin</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+H%2E+Foo%22">J. H. Foo</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+T%2E+Forcolin%22">G. T. Forcolin</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Formica%22">A. Formica</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+A%2E+Förster%22">F. A. Förster</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+C%2E+Forti%22">A. C. Forti</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+G%2E+Foster%22">A. G. Foster</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+G%2E+Foti%22">M. G. Foti</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Fournier%22">D. Fournier</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+Fox%22">H. Fox</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Francavilla%22">P. Francavilla</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Francescato%22">S. Francescato</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Franchini%22">M. Franchini</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Franchino%22">S. Franchino</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Francis%22">D. Francis</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Franconi%22">L. Franconi</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Franklin%22">M. Franklin</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+N%2E+Fray%22">A. N. Fray</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+M%2E+Freeman%22">P. M. Freeman</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Freund%22">B. Freund</searchLink><br /><searchLink fieldCode="AR" term="%22W%2E+S%2E+Freund%22">W. S. Freund</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+M%2E+Freundlich%22">E. M. Freundlich</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+C%2E+Frizzell%22">D. C. Frizzell</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Froidevaux%22">D. Froidevaux</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+A%2E+Frost%22">J. A. Frost</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Fukunaga%22">C. Fukunaga</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Fullana+Torregrosa%22">E. Fullana Torregrosa</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Fumagalli%22">E. Fumagalli</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Fusayasu%22">T. Fusayasu</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Fuster%22">J. Fuster</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Gabrielli%22">A. Gabrielli</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Gadatsch%22">S. Gadatsch</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Gadow%22">P. Gadow</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Gagliardi%22">G. Gagliardi</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+G%2E+Gagnon%22">L. G. Gagnon</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Galea%22">C. Galea</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Galhardo%22">B. Galhardo</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+E%2E+Gallardo%22">G. E. Gallardo</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+J%2E+Gallas%22">E. J. Gallas</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+J%2E+Gallop%22">B. J. Gallop</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Galster%22">G. Galster</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Gamboa+Goni%22">R. Gamboa Goni</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+K%2E+Gan%22">K. K. Gan</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Ganguly%22">S. Ganguly</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Gao%22">J. Gao</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+Gao%22">Y. Gao</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+S%2E+Gao%22">Y. S. Gao</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+García%22">C. García</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+E%2E+García+Navarro%22">J. E. García Navarro</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+A%2E+García+Pascual%22">J. A. García Pascual</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Garcia-Argos%22">C. Garcia-Argos</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Garcia-Sciveres%22">M. Garcia-Sciveres</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+W%2E+Gardner%22">R. W. Gardner</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+Garelli%22">N. Garelli</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Gargiulo%22">S. Gargiulo</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+A%2E+Garner%22">C. A. Garner</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+Garonne%22">V. Garonne</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+J%2E+Gasiorowski%22">S. J. Gasiorowski</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Gaspar%22">P. Gaspar</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Gaudiello%22">A. Gaudiello</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Gaudio%22">G. Gaudio</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+L%2E+Gavrilenko%22">I. L. Gavrilenko</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Gavrilyuk%22">A. Gavrilyuk</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Gay%22">C. Gay</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Gaycken%22">G. Gaycken</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+N%2E+Gazis%22">E. N. Gazis</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+A%2E+Geanta%22">A. A. Geanta</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+M%2E+Gee%22">C. M. Gee</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+N%2E+P%2E+Gee%22">C. N. P. Gee</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Geisen%22">J. Geisen</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Geisen%22">M. Geisen</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Gemme%22">C. Gemme</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+H%2E+Genest%22">M. H. Genest</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Geng%22">C. Geng</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Gentile%22">S. Gentile</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+George%22">S. George</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Geralis%22">T. Geralis</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+O%2E+Gerlach%22">L. O. Gerlach</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Gessinger-Befurt%22">P. Gessinger-Befurt</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Gessner%22">G. Gessner</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Ghasemi%22">S. Ghasemi</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Ghasemi+Bostanabad%22">M. Ghasemi Bostanabad</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Ghneimat%22">M. Ghneimat</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Ghosh%22">A. Ghosh</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Giacobbe%22">B. Giacobbe</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Giagu%22">S. Giagu</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+Giangiacomi%22">N. Giangiacomi</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Giannetti%22">P. Giannetti</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Giannini%22">A. Giannini</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Giannini%22">G. Giannini</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+M%2E+Gibson%22">S. M. Gibson</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Gignac%22">M. Gignac</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Gillberg%22">D. Gillberg</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Gilles%22">G. Gilles</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+M%2E+Gingrich%22">D. M. Gingrich</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+P%2E+Giordani%22">M. P. Giordani</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+M%2E+Giorgi%22">F. M. Giorgi</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+F%2E+Giraud%22">P. F. Giraud</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Giugliarelli%22">G. Giugliarelli</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Giugni%22">D. Giugni</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Giuli%22">F. Giuli</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Gkaitatzis%22">S. Gkaitatzis</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+Gkialas%22">I. Gkialas</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+L%2E+Gkougkousis%22">E. L. Gkougkousis</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Gkountoumis%22">P. Gkountoumis</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+K%2E+Gladilin%22">L. K. Gladilin</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Glasman%22">C. Glasman</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Glatzer%22">J. Glatzer</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+C%2E+F%2E+Glaysher%22">P. C. F. Glaysher</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Glazov%22">A. Glazov</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+R%2E+Gledhill%22">G. R. Gledhill</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Goblirsch-Kolb%22">M. Goblirsch-Kolb</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Godin%22">D. Godin</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Goldfarb%22">S. Goldfarb</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Golling%22">T. Golling</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Golubkov%22">D. Golubkov</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Gomes%22">A. Gomes</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Goncalves+Gama%22">R. Goncalves Gama</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Gonçalo%22">R. Gonçalo</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Gonella%22">G. Gonella</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Gonella%22">L. Gonella</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Gongadze%22">A. Gongadze</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Gonnella%22">F. Gonnella</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+L%2E+Gonski%22">J. L. Gonski</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+González+de+la+Hoz%22">S. González de la Hoz</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Gonzalez-Sevilla%22">S. Gonzalez-Sevilla</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+R%2E+Gonzalvo+Rodriguez%22">G. R. Gonzalvo Rodriguez</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Goossens%22">L. Goossens</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+A%2E+Gorasia%22">N. A. Gorasia</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+A%2E+Gorbounov%22">P. A. Gorbounov</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+A%2E+Gordon%22">H. A. Gordon</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Gorini%22">B. Gorini</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Gorini%22">E. Gorini</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Gorišek%22">A. Gorišek</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+T%2E+Goshaw%22">A. T. Goshaw</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+I%2E+Gostkin%22">M. I. Gostkin</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+A%2E+Gottardo%22">C. A. Gottardo</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Gouighri%22">M. Gouighri</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Goujdami%22">D. Goujdami</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+G%2E+Goussiou%22">A. G. Goussiou</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+Govender%22">N. Govender</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Goy%22">C. Goy</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Gozani%22">E. Gozani</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+Grabowska-Bold%22">I. Grabowska-Bold</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+C%2E+Graham%22">E. C. Graham</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Gramling%22">J. Gramling</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Gramstad%22">E. Gramstad</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Grancagnolo%22">S. Grancagnolo</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Grandi%22">M. Grandi</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+Gratchev%22">V. Gratchev</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+M%2E+Gravila%22">P. M. Gravila</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+G%2E+Gravili%22">F. G. Gravili</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Gray%22">C. Gray</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+M%2E+Gray%22">H. M. Gray</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Grefe%22">C. Grefe</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Gregersen%22">K. Gregersen</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+M%2E+Gregor%22">I. M. Gregor</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Grenier%22">P. Grenier</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Grevtsov%22">K. Grevtsov</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Grieco%22">C. Grieco</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+A%2E+Grieser%22">N. A. Grieser</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+A%2E+Grillo%22">A. A. Grillo</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Grimm%22">K. Grimm</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Grinstein%22">S. Grinstein</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E-F%2E+Grivaz%22">J.-F. Grivaz</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Groh%22">S. Groh</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Gross%22">E. Gross</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Grosse-Knetter%22">J. Grosse-Knetter</searchLink><br /><searchLink fieldCode="AR" term="%22Z%2E+J%2E+Grout%22">Z. J. Grout</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Grud%22">C. Grud</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Grummer%22">A. Grummer</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Guan%22">L. Guan</searchLink><br /><searchLink fieldCode="AR" term="%22W%2E+Guan%22">W. Guan</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Gubbels%22">C. Gubbels</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Guenther%22">J. Guenther</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Guerguichon%22">A. Guerguichon</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+G%2E+R%2E+Guerrero+Rojas%22">J. G. R. Guerrero Rojas</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Guescini%22">F. Guescini</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Guest%22">D. Guest</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Gugel%22">R. Gugel</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Guillemin%22">T. Guillemin</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Guindon%22">S. Guindon</searchLink><br /><searchLink fieldCode="AR" term="%22U%2E+Gul%22">U. Gul</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Guo%22">J. Guo</searchLink><br /><searchLink fieldCode="AR" term="%22W%2E+Guo%22">W. Guo</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+Guo%22">Y. Guo</searchLink><br /><searchLink fieldCode="AR" term="%22Z%2E+Guo%22">Z. Guo</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Gupta%22">R. Gupta</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Gurbuz%22">S. Gurbuz</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Gustavino%22">G. Gustavino</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Guth%22">M. Guth</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Gutierrez%22">P. Gutierrez</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Gutschow%22">C. Gutschow</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Guyot%22">C. Guyot</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Gwenlan%22">C. Gwenlan</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+B%2E+Gwilliam%22">C. B. Gwilliam</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Haas%22">A. Haas</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Haber%22">C. Haber</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+K%2E+Hadavand%22">H. K. Hadavand</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+Haddad%22">N. Haddad</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Hadef%22">A. Hadef</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Hageböck%22">S. Hageböck</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Haleem%22">M. Haleem</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Haley%22">J. Haley</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Halladjian%22">G. Halladjian</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+D%2E+Hallewell%22">G. D. Hallewell</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Hamacher%22">K. Hamacher</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Hamal%22">P. Hamal</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Hamano%22">K. Hamano</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+Hamdaoui%22">H. Hamdaoui</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Hamer%22">M. Hamer</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+N%2E+Hamity%22">G. N. Hamity</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Han%22">K. Han</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Han%22">L. Han</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Han%22">S. Han</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+F%2E+Han%22">Y. F. Han</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Hanagaki%22">K. Hanagaki</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Hance%22">M. Hance</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+M%2E+Handl%22">D. M. Handl</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Haney%22">B. Haney</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Hankache%22">R. Hankache</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Hansen%22">E. Hansen</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+B%2E+Hansen%22">J. B. Hansen</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+D%2E+Hansen%22">J. D. Hansen</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+C%2E+Hansen%22">M. C. Hansen</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+H%2E+Hansen%22">P. H. Hansen</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+C%2E+Hanson%22">E. C. Hanson</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Hara%22">K. Hara</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Harenberg%22">T. Harenberg</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Harkusha%22">S. Harkusha</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+F%2E+Harrison%22">P. F. Harrison</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+M%2E+Hartmann%22">N. M. Hartmann</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+Hasegawa%22">Y. Hasegawa</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Hasib%22">A. Hasib</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Hassani%22">S. Hassani</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Haug%22">S. Haug</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Hauser%22">R. Hauser</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+B%2E+Havener%22">L. B. Havener</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Havranek%22">M. Havranek</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+M%2E+Hawkes%22">C. M. Hawkes</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+J%2E+Hawkings%22">R. J. Hawkings</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Hayden%22">D. Hayden</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Hayes%22">C. Hayes</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+L%2E+Hayes%22">R. L. Hayes</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+P%2E+Hays%22">C. P. Hays</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+M%2E+Hays%22">J. M. Hays</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+S%2E+Hayward%22">H. S. Hayward</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+J%2E+Haywood%22">S. J. Haywood</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+He%22">F. He</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+P%2E+Heath%22">M. P. Heath</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+Hedberg%22">V. Hedberg</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Heelan%22">L. Heelan</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Heer%22">S. Heer</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+K%2E+Heidegger%22">K. K. Heidegger</searchLink><br /><searchLink fieldCode="AR" term="%22W%2E+D%2E+Heidorn%22">W. D. Heidorn</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Heilman%22">J. Heilman</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Heim%22">S. Heim</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Heim%22">T. Heim</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Heinemann%22">B. Heinemann</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+J%2E+Heinrich%22">J. J. Heinrich</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Heinrich%22">L. Heinrich</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Hejbal%22">J. Hejbal</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Helary%22">L. Helary</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Held%22">A. Held</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Hellesund%22">S. Hellesund</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+M%2E+Helling%22">C. M. Helling</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Hellman%22">S. Hellman</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Helsens%22">C. Helsens</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+C%2E+W%2E+Henderson%22">R. C. W. Henderson</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+Heng%22">Y. Heng</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Henkelmann%22">L. Henkelmann</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Henkelmann%22">S. Henkelmann</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+M%2E+Henriques+Correia%22">A. M. Henriques Correia</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+H%2E+Herbert%22">G. H. Herbert</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+Herde%22">H. Herde</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+Herget%22">V. Herget</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+Hernández+Jiménez%22">Y. Hernández Jiménez</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+Herr%22">H. Herr</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+G%2E+Herrmann%22">M. G. Herrmann</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Herrmann%22">T. Herrmann</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Herten%22">G. Herten</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Hertenberger%22">R. Hertenberger</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Hervas%22">L. Hervas</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+C%2E+Herwig%22">T. C. Herwig</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+G%2E+Hesketh%22">G. G. Hesketh</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+P%2E+Hessey%22">N. P. Hessey</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Higashida%22">A. Higashida</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Higashino%22">S. Higashino</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Higón-Rodriguez%22">E. Higón-Rodriguez</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Hildebrand%22">K. Hildebrand</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Hill%22">E. Hill</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+C%2E+Hill%22">J. C. Hill</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+K%2E+Hill%22">K. K. Hill</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+H%2E+Hiller%22">K. H. Hiller</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+J%2E+Hillier%22">S. J. Hillier</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Hils%22">M. Hils</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+Hinchliffe%22">I. Hinchliffe</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Hinterkeuser%22">F. Hinterkeuser</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Hirose%22">M. Hirose</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Hirose%22">S. Hirose</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Hirschbuehl%22">D. Hirschbuehl</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Hiti%22">B. Hiti</searchLink><br /><searchLink fieldCode="AR" term="%22O%2E+Hladik%22">O. Hladik</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+R%2E+Hlaluku%22">D. R. Hlaluku</searchLink><br /><searchLink fieldCode="AR" term="%22X%2E+Hoad%22">X. Hoad</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Hobbs%22">J. Hobbs</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+Hod%22">N. Hod</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+C%2E+Hodgkinson%22">M. C. Hodgkinson</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Hoecker%22">A. Hoecker</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Hohn%22">D. Hohn</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Hohov%22">D. Hohov</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Holm%22">T. Holm</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+R%2E+Holmes%22">T. R. Holmes</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Holzbock%22">M. Holzbock</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+B%2E+A%2E+H%2E+Hommels%22">L. B. A. H. Hommels</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Honda%22">S. Honda</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+M%2E+Hong%22">T. M. Hong</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+C%2E+Honig%22">J. C. Honig</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Hönle%22">A. Hönle</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+H%2E+Hooberman%22">B. H. Hooberman</searchLink><br /><searchLink fieldCode="AR" term="%22W%2E+H%2E+Hopkins%22">W. H. Hopkins</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+Horii%22">Y. Horii</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Horn%22">P. Horn</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+A%2E+Horyn%22">L. A. Horyn</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Hou%22">S. Hou</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Hoummada%22">A. Hoummada</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Howarth%22">J. Howarth</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Hoya%22">J. Hoya</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Hrabovsky%22">M. Hrabovsky</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Hrdinka%22">J. Hrdinka</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+Hristova%22">I. Hristova</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Hrivnac%22">J. Hrivnac</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Hrynevich%22">A. Hrynevich</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Hryn%27ova%22">T. Hryn’ova</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+J%2E+Hsu%22">P. J. Hsu</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E-C%2E+Hsu%22">S.-C. Hsu</searchLink><br /><searchLink fieldCode="AR" term="%22Q%2E+Hu%22">Q. Hu</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Hu%22">S. Hu</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+F%2E+Hu%22">Y. F. Hu</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+P%2E+Huang%22">D. P. Huang</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+Huang%22">Y. Huang</searchLink><br /><searchLink fieldCode="AR" term="%22Z%2E+Hubacek%22">Z. Hubacek</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Hubaut%22">F. Hubaut</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Huebner%22">M. Huebner</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Huegging%22">F. Huegging</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+B%2E+Huffman%22">T. B. Huffman</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Huhtinen%22">M. Huhtinen</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+F%2E+H%2E+Hunter%22">R. F. H. Hunter</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Huo%22">P. Huo</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+M%2E+Hupe%22">A. M. Hupe</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+Huseynov%22">N. Huseynov</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Huston%22">J. Huston</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Huth%22">J. Huth</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Hyneman%22">R. Hyneman</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Hyrych%22">S. Hyrych</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Iacobucci%22">G. Iacobucci</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Iakovidis%22">G. Iakovidis</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+Ibragimov%22">I. Ibragimov</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Iconomidou-Fayard%22">L. Iconomidou-Fayard</searchLink><br /><searchLink fieldCode="AR" term="%22Z%2E+Idrissi%22">Z. Idrissi</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Iengo%22">P. Iengo</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Ignazzi%22">R. Ignazzi</searchLink><br /><searchLink fieldCode="AR" term="%22O%2E+Igonkina%22">O. Igonkina</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Iguchi%22">R. Iguchi</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Iizawa%22">T. Iizawa</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+Ikegami%22">Y. Ikegami</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Ikeno%22">M. Ikeno</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Iliadis%22">D. Iliadis</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+Ilic%22">N. Ilic</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Iltzsche%22">F. Iltzsche</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Introzzi%22">G. Introzzi</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Iodice%22">M. Iodice</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Iordanidou%22">K. Iordanidou</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+Ippolito%22">V. Ippolito</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+F%2E+Isacson%22">M. F. Isacson</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Ishino%22">M. Ishino</searchLink><br /><searchLink fieldCode="AR" term="%22W%2E+Islam%22">W. Islam</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Issever%22">C. Issever</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Istin%22">S. Istin</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Ito%22">F. Ito</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+M%2E+Iturbe+Ponce%22">J. M. Iturbe Ponce</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Iuppa%22">R. Iuppa</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Ivina%22">A. Ivina</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+Iwasaki%22">H. Iwasaki</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+M%2E+Izen%22">J. M. Izen</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+Izzo%22">V. Izzo</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Jacka%22">P. Jacka</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Jackson%22">P. Jackson</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+M%2E+Jacobs%22">R. M. Jacobs</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+P%2E+Jaeger%22">B. P. Jaeger</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+Jain%22">V. Jain</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Jäkel%22">G. Jäkel</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+B%2E+Jakobi%22">K. B. Jakobi</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Jakobs%22">K. Jakobs</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Jakoubek%22">T. Jakoubek</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Jamieson%22">J. Jamieson</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+W%2E+Janas%22">K. W. Janas</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Jansky%22">R. Jansky</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Janssen%22">J. Janssen</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Janus%22">M. Janus</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+A%2E+Janus%22">P. A. Janus</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Jarlskog%22">G. Jarlskog</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+Javadov%22">N. Javadov</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Javůrek%22">T. Javůrek</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Javurkova%22">M. Javurkova</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Jeanneau%22">F. Jeanneau</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Jeanty%22">L. Jeanty</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Jejelava%22">J. Jejelava</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Jelinskas%22">A. Jelinskas</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Jenni%22">P. Jenni</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Jeong%22">J. Jeong</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+Jeong%22">N. Jeong</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Jézéquel%22">S. Jézéquel</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+Ji%22">H. Ji</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Jia%22">J. Jia</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+Jiang%22">H. Jiang</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+Jiang%22">Y. Jiang</searchLink><br /><searchLink fieldCode="AR" term="%22Z%2E+Jiang%22">Z. Jiang</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Jiggins%22">S. Jiggins</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+A%2E+Jimenez+Morales%22">F. A. Jimenez Morales</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Jimenez+Pena%22">J. Jimenez Pena</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Jin%22">S. Jin</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Jinaru%22">A. Jinaru</searchLink><br /><searchLink fieldCode="AR" term="%22O%2E+Jinnouchi%22">O. Jinnouchi</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+Jivan%22">H. Jivan</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Johansson%22">P. Johansson</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+A%2E+Johns%22">K. A. Johns</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+A%2E+Johnson%22">C. A. Johnson</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Jon-And%22">K. Jon-And</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+W%2E+L%2E+Jones%22">R. W. L. Jones</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+D%2E+Jones%22">S. D. Jones</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Jones%22">S. Jones</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+J%2E+Jones%22">T. J. Jones</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Jongmanns%22">J. Jongmanns</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+M%2E+Jorge%22">P. M. Jorge</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Jovicevic%22">J. Jovicevic</searchLink><br /><searchLink fieldCode="AR" term="%22X%2E+Ju%22">X. Ju</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+J%2E+Junggeburth%22">J. J. Junggeburth</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Juste+Rozas%22">A. Juste Rozas</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Kaczmarska%22">A. Kaczmarska</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Kado%22">M. Kado</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+Kagan%22">H. Kagan</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Kagan%22">M. Kagan</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Kahn%22">A. Kahn</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Kahra%22">C. Kahra</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Kaji%22">T. Kaji</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Kajomovitz%22">E. Kajomovitz</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+W%2E+Kalderon%22">C. W. Kalderon</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Kaluza%22">A. Kaluza</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Kamenshchikov%22">A. Kamenshchikov</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Kaneda%22">M. Kaneda</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+J%2E+Kang%22">N. J. Kang</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Kanjir%22">L. Kanjir</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+Kano%22">Y. Kano</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+A%2E+Kantserov%22">V. A. Kantserov</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Kanzaki%22">J. Kanzaki</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+S%2E+Kaplan%22">L. S. Kaplan</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Kar%22">D. Kar</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Karava%22">K. Karava</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+J%2E+Kareem%22">M. J. Kareem</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+N%2E+Karpov%22">S. N. Karpov</searchLink><br /><searchLink fieldCode="AR" term="%22Z%2E+M%2E+Karpova%22">Z. M. Karpova</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+Kartvelishvili%22">V. Kartvelishvili</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+N%2E+Karyukhin%22">A. N. Karyukhin</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Kashif%22">L. Kashif</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+D%2E+Kass%22">R. D. Kass</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Kastanas%22">A. Kastanas</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Kato%22">C. Kato</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Katzy%22">J. Katzy</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Kawade%22">K. Kawade</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Kawagoe%22">K. Kawagoe</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Kawaguchi%22">T. Kawaguchi</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Kawamoto%22">T. Kawamoto</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Kawamura%22">G. Kawamura</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+F%2E+Kay%22">E. F. Kay</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+F%2E+Kazanin%22">V. F. Kazanin</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Keeler%22">R. Keeler</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Kehoe%22">R. Kehoe</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+S%2E+Keller%22">J. S. Keller</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Kellermann%22">E. Kellermann</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Kelsey%22">D. Kelsey</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+J%2E+Kempster%22">J. J. Kempster</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Kendrick%22">J. Kendrick</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+E%2E+Kennedy%22">K. E. Kennedy</searchLink><br /><searchLink fieldCode="AR" term="%22O%2E+Kepka%22">O. Kepka</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Kersten%22">S. Kersten</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+P%2E+Kerševan%22">B. P. Kerševan</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Ketabchi+Haghighat%22">S. Ketabchi Haghighat</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Khader%22">M. Khader</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Khalil-Zada%22">F. Khalil-Zada</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Khandoga%22">M. Khandoga</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Khanov%22">A. Khanov</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+G%2E+Kharlamov%22">A. G. Kharlamov</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Kharlamova%22">T. Kharlamova</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+E%2E+Khoda%22">E. E. Khoda</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Khodinov%22">A. Khodinov</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+J%2E+Khoo%22">T. J. Khoo</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Khramov%22">E. Khramov</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Khubua%22">J. Khubua</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Kido%22">S. Kido</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Kiehn%22">M. Kiehn</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+R%2E+Kilby%22">C. R. Kilby</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+K%2E+Kim%22">Y. K. Kim</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+Kimura%22">N. Kimura</searchLink><br /><searchLink fieldCode="AR" term="%22O%2E+M%2E+Kind%22">O. M. Kind</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+T%2E+King%22">B. T. King</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Kirchmeier%22">D. Kirchmeier</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Kirk%22">J. Kirk</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+E%2E+Kiryunin%22">A. E. Kiryunin</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Kishimoto%22">T. Kishimoto</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+P%2E+Kisliuk%22">D. P. Kisliuk</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+Kitali%22">V. Kitali</searchLink><br /><searchLink fieldCode="AR" term="%22O%2E+Kivernyk%22">O. Kivernyk</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Klapdor-Kleingrothaus%22">T. Klapdor-Kleingrothaus</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Klassen%22">M. Klassen</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+H%2E+Klein%22">M. H. Klein</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Klein%22">M. Klein</searchLink><br /><searchLink fieldCode="AR" term="%22U%2E+Klein%22">U. Klein</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Kleinknecht%22">K. Kleinknecht</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Klimek%22">P. Klimek</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Klimentov%22">A. Klimentov</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Klingl%22">T. Klingl</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Klioutchnikova%22">T. Klioutchnikova</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+F%2E+Klitzner%22">F. F. Klitzner</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Kluit%22">P. Kluit</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Kluth%22">S. Kluth</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Kneringer%22">E. Kneringer</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+B%2E+F%2E+G%2E+Knoops%22">E. B. F. G. Knoops</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Knue%22">A. Knue</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Kobayashi%22">D. Kobayashi</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Kobayashi%22">T. Kobayashi</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Kobel%22">M. Kobel</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Kocian%22">M. Kocian</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Kodys%22">P. Kodys</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+T%2E+Koenig%22">P. T. Koenig</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Koffas%22">T. Koffas</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+M%2E+Köhler%22">N. M. Köhler</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Koi%22">T. Koi</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Kolb%22">M. Kolb</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+Koletsou%22">I. Koletsou</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Komarek%22">T. Komarek</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Kondo%22">T. Kondo</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Köneke%22">K. Köneke</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+X%2E+Y%2E+Kong%22">A. X. Y. Kong</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+C%2E+König%22">A. C. König</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Kono%22">T. Kono</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Konoplich%22">R. Konoplich</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+Konstantinides%22">V. Konstantinides</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+Konstantinidis%22">N. Konstantinidis</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Konya%22">B. Konya</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Kopeliansky%22">R. Kopeliansky</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Koperny%22">S. Koperny</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Korcyl%22">K. Korcyl</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Kordas%22">K. Kordas</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Koren%22">G. Koren</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Korn%22">A. Korn</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+Korolkov%22">I. Korolkov</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+V%2E+Korolkova%22">E. V. Korolkova</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+Korotkova%22">N. Korotkova</searchLink><br /><searchLink fieldCode="AR" term="%22O%2E+Kortner%22">O. Kortner</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Kortner%22">S. Kortner</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Kosek%22">T. Kosek</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+V%2E+Kostyukhin%22">V. V. Kostyukhin</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Kotsokechagia%22">A. Kotsokechagia</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Kotwal%22">A. Kotwal</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Koulouris%22">A. Koulouris</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Kourkoumeli-Charalampidi%22">A. Kourkoumeli-Charalampidi</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Kourkoumelis%22">C. Kourkoumelis</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Kourlitis%22">E. Kourlitis</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+Kouskoura%22">V. Kouskoura</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+B%2E+Kowalewska%22">A. B. Kowalewska</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Kowalewski%22">R. Kowalewski</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Kozakai%22">C. Kozakai</searchLink><br /><searchLink fieldCode="AR" term="%22W%2E+Kozanecki%22">W. Kozanecki</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+S%2E+Kozhin%22">A. S. Kozhin</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+A%2E+Kramarenko%22">V. A. Kramarenko</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Kramberger%22">G. Kramberger</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Krasnopevtsev%22">D. Krasnopevtsev</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+W%2E+Krasny%22">M. W. Krasny</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Krasznahorkay%22">A. Krasznahorkay</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Krauss%22">D. Krauss</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+A%2E+Kremer%22">J. A. Kremer</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Kretzschmar%22">J. Kretzschmar</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Krieger%22">P. Krieger</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Krieter%22">F. Krieter</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Krishnan%22">A. Krishnan</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Krizka%22">K. Krizka</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Kroeninger%22">K. Kroeninger</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+Kroha%22">H. Kroha</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Kroll%22">J. Kroll</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+S%2E+Krowpman%22">K. S. Krowpman</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Krstic%22">J. Krstic</searchLink><br /><searchLink fieldCode="AR" term="%22U%2E+Kruchonak%22">U. Kruchonak</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+Krüger%22">H. Krüger</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+Krumnack%22">N. Krumnack</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+C%2E+Kruse%22">M. C. Kruse</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+A%2E+Krzysiak%22">J. A. Krzysiak</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Kubota%22">T. Kubota</searchLink><br /><searchLink fieldCode="AR" term="%22O%2E+Kuchinskaia%22">O. Kuchinskaia</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Kuday%22">S. Kuday</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+T%2E+Kuechler%22">J. T. Kuechler</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Kuehn%22">S. Kuehn</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Kugel%22">A. Kugel</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Kuhl%22">T. Kuhl</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+Kukhtin%22">V. Kukhtin</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Kukla%22">R. Kukla</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+Kulchitsky%22">Y. Kulchitsky</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Kuleshov%22">S. Kuleshov</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+P%2E+Kulinich%22">Y. P. Kulinich</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Kuna%22">M. Kuna</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Kunigo%22">T. Kunigo</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Kupco%22">A. Kupco</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Kupfer%22">T. Kupfer</searchLink><br /><searchLink fieldCode="AR" term="%22O%2E+Kuprash%22">O. Kuprash</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+Kurashige%22">H. Kurashige</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+L%2E+Kurchaninov%22">L. L. Kurchaninov</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+A%2E+Kurochkin%22">Y. A. Kurochkin</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Kurova%22">A. Kurova</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+G%2E+Kurth%22">M. G. Kurth</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+S%2E+Kuwertz%22">E. S. Kuwertz</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Kuze%22">M. Kuze</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+K%2E+Kvam%22">A. K. Kvam</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Kvita%22">J. Kvita</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Kwan%22">T. Kwan</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+La+Rosa%22">A. La Rosa</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+La+Rotonda%22">L. La Rotonda</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+La+Ruffa%22">F. La Ruffa</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Lacasta%22">C. Lacasta</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Lacava%22">F. Lacava</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+P%2E+J%2E+Lack%22">D. P. J. Lack</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+Lacker%22">H. Lacker</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Lacour%22">D. Lacour</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Ladygin%22">E. Ladygin</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Lafaye%22">R. Lafaye</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Laforge%22">B. Laforge</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Lagouri%22">T. Lagouri</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Lai%22">S. Lai</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+K%2E+Lakomiec%22">I. K. Lakomiec</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Lammers%22">S. Lammers</searchLink><br /><searchLink fieldCode="AR" term="%22W%2E+Lampl%22">W. Lampl</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Lampoudis%22">C. Lampoudis</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Lançon%22">E. Lançon</searchLink><br /><searchLink fieldCode="AR" term="%22U%2E+Landgraf%22">U. Landgraf</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+P%2E+J%2E+Landon%22">M. P. J. Landon</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+C%2E+Lanfermann%22">M. C. Lanfermann</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+S%2E+Lang%22">V. S. Lang</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+C%2E+Lange%22">J. C. Lange</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+J%2E+Langenberg%22">R. J. Langenberg</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+J%2E+Lankford%22">A. J. Lankford</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Lanni%22">F. Lanni</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Lantzsch%22">K. Lantzsch</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Lanza%22">A. Lanza</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Lapertosa%22">A. Lapertosa</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Laplace%22">S. Laplace</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+F%2E+Laporte%22">J. F. Laporte</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Lari%22">T. Lari</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Lasagni+Manghi%22">F. Lasagni Manghi</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Lassnig%22">M. Lassnig</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+S%2E+Lau%22">T. S. Lau</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Laudrain%22">A. Laudrain</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Laurier%22">A. Laurier</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Lavorgna%22">M. Lavorgna</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+D%2E+Lawlor%22">S. D. Lawlor</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Lazzaroni%22">M. Lazzaroni</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Le%22">B. Le</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Le+Guirriec%22">E. Le Guirriec</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+LeBlanc%22">M. LeBlanc</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+LeCompte%22">T. LeCompte</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Ledroit-Guillon%22">F. Ledroit-Guillon</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+C%2E+A%2E+Lee%22">A. C. A. Lee</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+A%2E+Lee%22">C. A. Lee</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+R%2E+Lee%22">G. R. Lee</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Lee%22">L. Lee</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+C%2E+Lee%22">S. C. Lee</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+J%2E+Lee%22">S. J. Lee</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Lee%22">S. Lee</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Lefebvre%22">B. Lefebvre</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+P%2E+Lefebvre%22">H. P. Lefebvre</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Lefebvre%22">M. Lefebvre</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Legger%22">F. Legger</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Leggett%22">C. Leggett</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Lehmann%22">K. Lehmann</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+Lehmann%22">N. Lehmann</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Lehmann+Miotto%22">G. Lehmann Miotto</searchLink><br /><searchLink fieldCode="AR" term="%22W%2E+A%2E+Leight%22">W. A. Leight</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Leisos%22">A. Leisos</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+A%2E+L%2E+Leite%22">M. A. L. Leite</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+E%2E+Leitgeb%22">C. E. Leitgeb</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Leitner%22">R. Leitner</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Lellouch%22">D. Lellouch</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+J%2E+C%2E+Leney%22">K. J. C. Leney</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Lenz%22">T. Lenz</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Leone%22">R. Leone</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Leone%22">S. Leone</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Leonidopoulos%22">C. Leonidopoulos</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Leopold%22">A. Leopold</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Leroy%22">C. Leroy</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Les%22">R. Les</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+G%2E+Lester%22">C. G. Lester</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Levchenko%22">M. Levchenko</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Levêque%22">J. Levêque</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Levin%22">D. Levin</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+J%2E+Levinson%22">L. J. Levinson</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+J%2E+Lewis%22">D. J. Lewis</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Li%22">B. Li</searchLink><br /><searchLink fieldCode="AR" term="%22C-Q%2E+Li%22">C-Q. Li</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Li%22">F. Li</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+Li%22">H. Li</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Li%22">J. Li</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Li%22">K. Li</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Li%22">L. Li</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Li%22">M. Li</searchLink><br /><searchLink fieldCode="AR" term="%22Q%2E+Li%22">Q. Li</searchLink><br /><searchLink fieldCode="AR" term="%22Q%2E+Y%2E+Li%22">Q. Y. Li</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Li%22">S. Li</searchLink><br /><searchLink fieldCode="AR" term="%22X%2E+Li%22">X. Li</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+Li%22">Y. Li</searchLink><br /><searchLink fieldCode="AR" term="%22Z%2E+Li%22">Z. Li</searchLink><br /><searchLink fieldCode="AR" term="%22Z%2E+Liang%22">Z. Liang</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Liberti%22">B. Liberti</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Liblong%22">A. Liblong</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Lie%22">K. Lie</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Lim%22">S. Lim</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Y%2E+Lin%22">C. Y. Lin</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Lin%22">K. Lin</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+H%2E+Lin%22">T. H. Lin</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+A%2E+Linck%22">R. A. Linck</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+H%2E+Lindon%22">J. H. Lindon</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+L%2E+Lionti%22">A. L. Lionti</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Lipeles%22">E. Lipeles</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Lipniacka%22">A. Lipniacka</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+M%2E+Liss%22">T. M. Liss</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Lister%22">A. Lister</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+M%2E+Litke%22">A. M. Litke</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+D%2E+Little%22">J. D. Little</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Liu%22">B. Liu</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+L%2E+Liu%22">B. L. Liu</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+B%2E+Liu%22">H. B. Liu</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+Liu%22">H. Liu</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+B%2E+Liu%22">J. B. Liu</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+K%2E+K%2E+Liu%22">J. K. K. Liu</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Liu%22">K. Liu</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Liu%22">M. Liu</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Liu%22">P. Liu</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+Liu%22">Y. Liu</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+L%2E+Liu%22">Y. L. Liu</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+W%2E+Liu%22">Y. W. Liu</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Livan%22">M. Livan</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Lleres%22">A. Lleres</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Llorente+Merino%22">J. Llorente Merino</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+L%2E+Lloyd%22">S. L. Lloyd</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Y%2E+Lo%22">C. Y. Lo</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Lo+Sterzo%22">F. Lo Sterzo</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+M%2E+Lobodzinska%22">E. M. Lobodzinska</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Loch%22">P. Loch</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Loffredo%22">S. Loffredo</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Lohse%22">T. Lohse</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Lohwasser%22">K. Lohwasser</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Lokajicek%22">M. Lokajicek</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+D%2E+Long%22">J. D. Long</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+E%2E+Long%22">R. E. Long</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Longo%22">L. Longo</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+A%2E+Looper%22">K. A. Looper</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+A%2E+Lopez%22">J. A. Lopez</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+Lopez+Paz%22">I. Lopez Paz</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Lopez+Solis%22">A. Lopez Solis</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Lorenz%22">J. Lorenz</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+Lorenzo+Martinez%22">N. Lorenzo Martinez</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+M%2E+Lory%22">A. M. Lory</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Losada%22">M. Losada</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+J%2E+Lösel%22">P. J. Lösel</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Lösle%22">A. Lösle</searchLink><br /><searchLink fieldCode="AR" term="%22X%2E+Lou%22">X. Lou</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Lounis%22">A. Lounis</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Love%22">J. Love</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+A%2E+Love%22">P. A. Love</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+J%2E+Lozano+Bahilo%22">J. J. Lozano Bahilo</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Lu%22">M. Lu</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+J%2E+Lu%22">Y. J. Lu</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+J%2E+Lubatti%22">H. J. Lubatti</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Luci%22">C. Luci</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Lucotte%22">A. Lucotte</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Luedtke%22">C. Luedtke</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Luehring%22">F. Luehring</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+Luise%22">I. Luise</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Luminari%22">L. Luminari</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Lund-Jensen%22">B. Lund-Jensen</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+S%2E+Lutz%22">M. S. Lutz</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Lynn%22">D. Lynn</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+Lyons%22">H. Lyons</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Lysak%22">R. Lysak</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Lytken%22">E. Lytken</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Lyu%22">F. Lyu</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+Lyubushkin%22">V. Lyubushkin</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Lyubushkina%22">T. Lyubushkina</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+Ma%22">H. Ma</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+L%2E+Ma%22">L. L. Ma</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+Ma%22">Y. Ma</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Maccarrone%22">G. Maccarrone</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Macchiolo%22">A. Macchiolo</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+M%2E+Macdonald%22">C. M. Macdonald</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Machado+Miguens%22">J. Machado Miguens</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Madaffari%22">D. Madaffari</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Madar%22">R. Madar</searchLink><br /><searchLink fieldCode="AR" term="%22W%2E+F%2E+Mader%22">W. F. Mader</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+Madysa%22">N. Madysa</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Maeda%22">J. Maeda</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Maeno%22">T. Maeno</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Maerker%22">M. Maerker</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+S%2E+Maevskiy%22">A. S. Maevskiy</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+Magerl%22">V. Magerl</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+Magini%22">N. Magini</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+J%2E+Mahon%22">D. J. Mahon</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Maidantchik%22">C. Maidantchik</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Maier%22">T. Maier</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Maio%22">A. Maio</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Maj%22">K. Maj</searchLink><br /><searchLink fieldCode="AR" term="%22O%2E+Majersky%22">O. Majersky</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Majewski%22">S. Majewski</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+Makida%22">Y. Makida</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+Makovec%22">N. Makovec</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Malaescu%22">B. Malaescu</searchLink><br /><searchLink fieldCode="AR" term="%22Pa%2E+Malecki%22">Pa. Malecki</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+P%2E+Maleev%22">V. P. Maleev</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Malek%22">F. Malek</searchLink><br /><searchLink fieldCode="AR" term="%22U%2E+Mallik%22">U. Mallik</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Malon%22">D. Malon</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Malone%22">C. Malone</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Maltezos%22">S. Maltezos</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Malyukov%22">S. Malyukov</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Mamuzic%22">J. Mamuzic</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Mancini%22">G. Mancini</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+Mandić%22">I. Mandić</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Manhaes+de+Andrade+Filho%22">L. Manhaes de Andrade Filho</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+M%2E+Maniatis%22">I. M. Maniatis</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Manjarres+Ramos%22">J. Manjarres Ramos</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+H%2E+Mankinen%22">K. H. Mankinen</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Mann%22">A. Mann</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Manousos%22">A. Manousos</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Mansoulie%22">B. Mansoulie</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+Manthos%22">I. Manthos</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Manzoni%22">S. Manzoni</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Marantis%22">A. Marantis</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Marceca%22">G. Marceca</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Marchese%22">L. Marchese</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Marchiori%22">G. Marchiori</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Marcisovsky%22">M. Marcisovsky</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Marcoccia%22">L. Marcoccia</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Marcon%22">C. Marcon</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+A%2E+Marin+Tobon%22">C. A. Marin Tobon</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Marjanovic%22">M. Marjanovic</searchLink><br /><searchLink fieldCode="AR" term="%22Z%2E+Marshall%22">Z. Marshall</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+U%2E+F%2E+Martensson%22">M. U. F. Martensson</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Marti-Garcia%22">S. Marti-Garcia</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+B%2E+Martin%22">C. B. Martin</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+A%2E+Martin%22">T. A. Martin</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+J%2E+Martin%22">V. J. Martin</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Martin+dit+Latour%22">B. Martin dit Latour</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Martinelli%22">L. Martinelli</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Martinez%22">M. Martinez</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+I%2E+Martinez+Outschoorn%22">V. I. Martinez Outschoorn</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Martin-Haugh%22">S. Martin-Haugh</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+S%2E+Martoiu%22">V. S. Martoiu</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+C%2E+Martyniuk%22">A. C. Martyniuk</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Marzin%22">A. Marzin</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+R%2E+Maschek%22">S. R. Maschek</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Masetti%22">L. Masetti</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Mashimo%22">T. Mashimo</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Mashinistov%22">R. Mashinistov</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Masik%22">J. Masik</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+L%2E+Maslennikov%22">A. L. Maslennikov</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Massa%22">L. Massa</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Massarotti%22">P. Massarotti</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Mastrandrea%22">P. Mastrandrea</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Mastroberardino%22">A. Mastroberardino</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Masubuchi%22">T. Masubuchi</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Matakias%22">D. Matakias</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Matic%22">A. Matic</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+Matsuzawa%22">N. Matsuzawa</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Mättig%22">P. Mättig</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Maurer%22">J. Maurer</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Maček%22">B. Maček</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+A%2E+Maximov%22">D. A. Maximov</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Mazini%22">R. Mazini</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+Maznas%22">I. Maznas</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+M%2E+Mazza%22">S. M. Mazza</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+P%2E+Mc+Kee%22">S. P. Mc Kee</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+G%2E+McCarthy%22">T. G. McCarthy</searchLink><br /><searchLink fieldCode="AR" term="%22W%2E+P%2E+McCormack%22">W. P. McCormack</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+F%2E+McDonald%22">E. F. McDonald</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+A%2E+Mcfayden%22">J. A. Mcfayden</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Mchedlidze%22">G. Mchedlidze</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+A%2E+McKay%22">M. A. McKay</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+D%2E+McLean%22">K. D. McLean</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+J%2E+McMahon%22">S. J. McMahon</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+C%2E+McNamara%22">P. C. McNamara</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+J%2E+McNicol%22">C. J. McNicol</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+A%2E+McPherson%22">R. A. McPherson</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+E%2E+Mdhluli%22">J. E. Mdhluli</searchLink><br /><searchLink fieldCode="AR" term="%22Z%2E+A%2E+Meadows%22">Z. A. Meadows</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Meehan%22">S. Meehan</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Megy%22">T. Megy</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Mehlhase%22">S. Mehlhase</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Mehta%22">A. Mehta</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Meideck%22">T. Meideck</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Meirose%22">B. Meirose</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Melini%22">D. Melini</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+R%2E+Mellado+Garcia%22">B. R. Mellado Garcia</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+D%2E+Mellenthin%22">J. D. Mellenthin</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Melo%22">M. Melo</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Meloni%22">F. Meloni</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Melzer%22">A. Melzer</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+B%2E+Menary%22">S. B. Menary</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+D%2E+Mendes+Gouveia%22">E. D. Mendes Gouveia</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Meng%22">L. Meng</searchLink><br /><searchLink fieldCode="AR" term="%22X%2E+T%2E+Meng%22">X. T. Meng</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Menke%22">S. Menke</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Meoni%22">E. Meoni</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Mergelmeyer%22">S. Mergelmeyer</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+A%2E+M%2E+Merkt%22">S. A. M. Merkt</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Merlassino%22">C. Merlassino</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Mermod%22">P. Mermod</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Merola%22">L. Merola</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Meroni%22">C. Meroni</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Merz%22">G. Merz</searchLink><br /><searchLink fieldCode="AR" term="%22O%2E+Meshkov%22">O. Meshkov</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+K%2E+R%2E+Meshreki%22">J. K. R. Meshreki</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Messina%22">A. Messina</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Metcalfe%22">J. Metcalfe</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+S%2E+Mete%22">A. S. Mete</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Meyer%22">C. Meyer</searchLink><br /><searchLink fieldCode="AR" term="%22J-P%2E+Meyer%22">J-P. Meyer</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+Meyer+Zu+Theenhausen%22">H. Meyer Zu Theenhausen</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Miano%22">F. Miano</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Michetti%22">M. Michetti</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+P%2E+Middleton%22">R. P. Middleton</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Mijović%22">L. Mijović</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Mikenberg%22">G. Mikenberg</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Mikestikova%22">M. Mikestikova</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Mikuž%22">M. Mikuž</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+Mildner%22">H. Mildner</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Milesi%22">M. Milesi</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Milic%22">A. Milic</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+A%2E+Millar%22">D. A. Millar</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+W%2E+Miller%22">D. W. Miller</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Milov%22">A. Milov</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+A%2E+Milstead%22">D. A. Milstead</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+A%2E+Mina%22">R. A. Mina</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+A%2E+Minaenko%22">A. A. Minaenko</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Miñano+Moya%22">M. Miñano Moya</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+A%2E+Minashvili%22">I. A. Minashvili</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+I%2E+Mincer%22">A. I. Mincer</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Mindur%22">B. Mindur</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Mineev%22">M. Mineev</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+Minegishi%22">Y. Minegishi</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+M%2E+Mir%22">L. M. Mir</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Mirto%22">A. Mirto</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+P%2E+Mistry%22">K. P. Mistry</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Mitani%22">T. Mitani</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Mitrevski%22">J. Mitrevski</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+A%2E+Mitsou%22">V. A. Mitsou</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Mittal%22">M. Mittal</searchLink><br /><searchLink fieldCode="AR" term="%22O%2E+Miu%22">O. Miu</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Miucci%22">A. Miucci</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+S%2E+Miyagawa%22">P. S. Miyagawa</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Mizukami%22">A. Mizukami</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+U%2E+Mjörnmark%22">J. U. Mjörnmark</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Mkrtchyan%22">T. Mkrtchyan</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Mlynarikova%22">M. Mlynarikova</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Moa%22">T. Moa</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Mochizuki%22">K. Mochizuki</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Mogg%22">P. Mogg</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Mohapatra%22">S. Mohapatra</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Moles-Valls%22">R. Moles-Valls</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+C%2E+Mondragon%22">M. C. Mondragon</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Mönig%22">K. Mönig</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Monk%22">J. Monk</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Monnier%22">E. Monnier</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Montalbano%22">A. Montalbano</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Montejo+Berlingen%22">J. Montejo Berlingen</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Montella%22">M. Montella</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Monticelli%22">F. Monticelli</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Monzani%22">S. Monzani</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+Morange%22">N. Morange</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Moreno%22">D. Moreno</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Moreno+Llácer%22">M. Moreno Llácer</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Moreno+Martinez%22">C. Moreno Martinez</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Morettini%22">P. Morettini</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Morgenstern%22">M. Morgenstern</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Morgenstern%22">S. Morgenstern</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Mori%22">D. Mori</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Morii%22">M. Morii</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Morinaga%22">M. Morinaga</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+Morisbak%22">V. Morisbak</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+K%2E+Morley%22">A. K. Morley</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Mornacchi%22">G. Mornacchi</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+P%2E+Morris%22">A. P. Morris</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Morvaj%22">L. Morvaj</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Moschovakos%22">P. Moschovakos</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Moser%22">B. Moser</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Mosidze%22">M. Mosidze</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Moskalets%22">T. Moskalets</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+J%2E+Moss%22">H. J. Moss</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Moss%22">J. Moss</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+J%2E+W%2E+Moyse%22">E. J. W. Moyse</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Muanza%22">S. Muanza</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Mueller%22">J. Mueller</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+S%2E+P%2E+Mueller%22">R. S. P. Mueller</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Muenstermann%22">D. Muenstermann</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+A%2E+Mullier%22">G. A. Mullier</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+P%2E+Mungo%22">D. P. Mungo</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+L%2E+Munoz+Martinez%22">J. L. Munoz Martinez</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+J%2E+Munoz+Sanchez%22">F. J. Munoz Sanchez</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Murin%22">P. Murin</searchLink><br /><searchLink fieldCode="AR" term="%22W%2E+J%2E+Murray%22">W. J. Murray</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Murrone%22">A. Murrone</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Muškinja%22">M. Muškinja</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Mwewa%22">C. Mwewa</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+G%2E+Myagkov%22">A. G. Myagkov</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+A%2E+Myers%22">A. A. Myers</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Myers%22">J. Myers</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Myska%22">M. Myska</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+P%2E+Nachman%22">B. P. Nachman</searchLink><br /><searchLink fieldCode="AR" term="%22O%2E+Nackenhorst%22">O. Nackenhorst</searchLink><br /><searchLink fieldCode="AR" term="%22A%2ENag+Nag%22">A.Nag Nag</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Nagai%22">K. Nagai</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Nagano%22">K. Nagano</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+Nagasaka%22">Y. Nagasaka</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+L%2E+Nagle%22">J. L. Nagle</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Nagy%22">E. Nagy</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+M%2E+Nairz%22">A. M. Nairz</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+Nakahama%22">Y. Nakahama</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Nakamura%22">K. Nakamura</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Nakamura%22">T. Nakamura</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+Nakano%22">I. Nakano</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+Nanjo%22">H. Nanjo</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Napolitano%22">F. Napolitano</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+F%2E+Naranjo+Garcia%22">R. F. Naranjo Garcia</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Narayan%22">R. Narayan</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+Naryshkin%22">I. Naryshkin</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Naumann%22">T. Naumann</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Navarro%22">G. Navarro</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Y%2E+Nechaeva%22">P. Y. Nechaeva</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Nechansky%22">F. Nechansky</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+J%2E+Neep%22">T. J. Neep</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Negri%22">A. Negri</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Negrini%22">M. Negrini</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Nellist%22">C. Nellist</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+E%2E+Nelson%22">M. E. Nelson</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Nemecek%22">S. Nemecek</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Nemethy%22">P. Nemethy</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Nessi%22">M. Nessi</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+S%2E+Neubauer%22">M. S. Neubauer</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Neumann%22">M. Neumann</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Newhouse%22">R. Newhouse</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+R%2E+Newman%22">P. R. Newman</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+S%2E+Ng%22">Y. S. Ng</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+W%2E+Y%2E+Ng%22">Y. W. Y. Ng</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Ngair%22">B. Ngair</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+D%2E+N%2E+Nguyen%22">H. D. N. Nguyen</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Nguyen+Manh%22">T. Nguyen Manh</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Nibigira%22">E. Nibigira</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+B%2E+Nickerson%22">R. B. Nickerson</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Nicolaidou%22">R. Nicolaidou</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+S%2E+Nielsen%22">D. S. Nielsen</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Nielsen%22">J. Nielsen</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+Nikiforou%22">N. Nikiforou</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+Nikolaenko%22">V. Nikolaenko</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+Nikolic-Audit%22">I. Nikolic-Audit</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Nikolopoulos%22">K. Nikolopoulos</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Nilsson%22">P. Nilsson</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+R%2E+Nindhito%22">H. R. Nindhito</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+Ninomiya%22">Y. Ninomiya</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Nisati%22">A. Nisati</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+Nishu%22">N. Nishu</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Nisius%22">R. Nisius</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+Nitsche%22">I. Nitsche</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Nitta%22">T. Nitta</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Nobe%22">T. Nobe</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+Noguchi%22">Y. Noguchi</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+Nomidis%22">I. Nomidis</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+A%2E+Nomura%22">M. A. Nomura</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Nordberg%22">M. Nordberg</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+Norjoharuddeen%22">N. Norjoharuddeen</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Novak%22">T. Novak</searchLink><br /><searchLink fieldCode="AR" term="%22O%2E+Novgorodova%22">O. Novgorodova</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Novotny%22">R. Novotny</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Nozka%22">L. Nozka</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Ntekas%22">K. Ntekas</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Nurse%22">E. Nurse</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+G%2E+Oakham%22">F. G. Oakham</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+Oberlack%22">H. Oberlack</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Ocariz%22">J. Ocariz</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Ochi%22">A. Ochi</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+Ochoa%22">I. Ochoa</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+P%2E+Ochoa-Ricoux%22">J. P. Ochoa-Ricoux</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+O%27Connor%22">K. O’Connor</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Oda%22">S. Oda</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Odaka%22">S. Odaka</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Oerdek%22">S. Oerdek</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Ogrodnik%22">A. Ogrodnik</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Oh%22">A. Oh</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+H%2E+Oh%22">S. H. Oh</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+C%2E+Ohm%22">C. C. Ohm</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+Oide%22">H. Oide</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+L%2E+Ojeda%22">M. L. Ojeda</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+Okawa%22">H. Okawa</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+Okazaki%22">Y. Okazaki</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+W%2E+O%27Keefe%22">M. W. O’Keefe</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+Okumura%22">Y. Okumura</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Okuyama%22">T. Okuyama</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Olariu%22">A. Olariu</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+F%2E+Oleiro+Seabra%22">L. F. Oleiro Seabra</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+A%2E+Olivares+Pino%22">S. A. Olivares Pino</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Oliveira+Damazio%22">D. Oliveira Damazio</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+L%2E+Oliver%22">J. L. Oliver</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+J%2E+R%2E+Olsson%22">M. J. R. Olsson</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Olszewski%22">A. Olszewski</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Olszowska%22">J. Olszowska</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+C%2E+O%27Neil%22">D. C. O’Neil</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+P%2E+O%27neill%22">A. P. O’neill</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Onofre%22">A. Onofre</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+U%2E+E%2E+Onyisi%22">P. U. E. Onyisi</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+Oppen%22">H. Oppen</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+J%2E+Oreglia%22">M. J. Oreglia</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+E%2E+Orellana%22">G. E. Orellana</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Orestano%22">D. Orestano</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+Orlando%22">N. Orlando</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+S%2E+Orr%22">R. S. Orr</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+O%27Shea%22">V. O’Shea</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Ospanov%22">R. Ospanov</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Otero+y+Garzon%22">G. Otero y Garzon</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+Otono%22">H. Otono</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+S%2E+Ott%22">P. S. Ott</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Ouchrif%22">M. Ouchrif</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Ouellette%22">J. Ouellette</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Ould-Saada%22">F. Ould-Saada</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Ouraou%22">A. Ouraou</searchLink><br /><searchLink fieldCode="AR" term="%22Q%2E+Ouyang%22">Q. Ouyang</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Owen%22">M. Owen</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+E%2E+Owen%22">R. E. Owen</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+E%2E+Ozcan%22">V. E. Ozcan</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+Ozturk%22">N. Ozturk</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Pacalt%22">J. Pacalt</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+A%2E+Pacey%22">H. A. Pacey</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Pachal%22">K. Pachal</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Pacheco+Pages%22">A. Pacheco Pages</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Padilla+Aranda%22">C. Padilla Aranda</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Pagan+Griso%22">S. Pagan Griso</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Paganini%22">M. Paganini</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Palacino%22">G. Palacino</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Palazzo%22">S. Palazzo</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Palestini%22">S. Palestini</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Palka%22">M. Palka</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Pallin%22">D. Pallin</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+Panagoulias%22">I. Panagoulias</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+E%2E+Pandini%22">C. E. Pandini</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+G%2E+Panduro+Vazquez%22">J. G. Panduro Vazquez</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Pani%22">P. Pani</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Panizzo%22">G. Panizzo</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Paolozzi%22">L. Paolozzi</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Papadatos%22">C. Papadatos</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Papageorgiou%22">K. Papageorgiou</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Parajuli%22">S. Parajuli</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Paramonov%22">A. Paramonov</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Paredes+Hernandez%22">D. Paredes Hernandez</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+R%2E+Paredes+Saenz%22">S. R. Paredes Saenz</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Parida%22">B. Parida</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+H%2E+Park%22">T. H. Park</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+J%2E+Parker%22">A. J. Parker</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+A%2E+Parker%22">M. A. Parker</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Parodi%22">F. Parodi</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+W%2E+Parrish%22">E. W. Parrish</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+A%2E+Parsons%22">J. A. Parsons</searchLink><br /><searchLink fieldCode="AR" term="%22U%2E+Parzefall%22">U. Parzefall</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Pascual+Dominguez%22">L. Pascual Dominguez</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+R%2E+Pascuzzi%22">V. R. Pascuzzi</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+M%2E+P%2E+Pasner%22">J. M. P. Pasner</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Pasquali%22">F. Pasquali</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Pasqualucci%22">E. Pasqualucci</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Passaggio%22">S. Passaggio</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Pastore%22">F. Pastore</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Pasuwan%22">P. Pasuwan</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Pataraia%22">S. Pataraia</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+R%2E+Pater%22">J. R. Pater</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Pathak%22">A. Pathak</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Pauly%22">T. Pauly</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Pearkes%22">J. Pearkes</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Pearson%22">B. Pearson</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Pedersen%22">M. Pedersen</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Pedraza+Diaz%22">L. Pedraza Diaz</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Pedro%22">R. Pedro</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Peiffer%22">T. Peiffer</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+V%2E+Peleganchuk%22">S. V. Peleganchuk</searchLink><br /><searchLink fieldCode="AR" term="%22O%2E+Penc%22">O. Penc</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+Peng%22">H. Peng</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+S%2E+Peralva%22">B. S. Peralva</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+M%2E+Perego%22">M. M. Perego</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+P%2E+Pereira+Peixoto%22">A. P. Pereira Peixoto</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+V%2E+Perepelitsa%22">D. V. Perepelitsa</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Peri%22">F. Peri</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Perini%22">L. Perini</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+Pernegger%22">H. Pernegger</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Perrella%22">S. Perrella</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Perrevoort%22">A. Perrevoort</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Peters%22">K. Peters</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+F%2E+Y%2E+Peters%22">R. F. Y. Peters</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+A%2E+Petersen%22">B. A. Petersen</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+C%2E+Petersen%22">T. C. Petersen</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Petit%22">E. Petit</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Petridis%22">A. Petridis</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Petridou%22">C. Petridou</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Petroff%22">P. Petroff</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Petrov%22">M. Petrov</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Petrucci%22">F. Petrucci</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Pettee%22">M. Pettee</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+E%2E+Pettersson%22">N. E. Pettersson</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Petukhova%22">K. Petukhova</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Peyaud%22">A. Peyaud</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Pezoa%22">R. Pezoa</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Pezzotti%22">L. Pezzotti</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Pham%22">T. Pham</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+H%2E+Phillips%22">F. H. Phillips</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+W%2E+Phillips%22">P. W. Phillips</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+W%2E+Phipps%22">M. W. Phipps</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Piacquadio%22">G. Piacquadio</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Pianori%22">E. Pianori</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Picazio%22">A. Picazio</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+H%2E+Pickles%22">R. H. Pickles</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Piegaia%22">R. Piegaia</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Pietreanu%22">D. Pietreanu</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+E%2E+Pilcher%22">J. E. Pilcher</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+D%2E+Pilkington%22">A. D. Pilkington</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Pinamonti%22">M. Pinamonti</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+L%2E+Pinfold%22">J. L. Pinfold</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Pitt%22">M. Pitt</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Pizzimento%22">L. Pizzimento</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E-A%2E+Pleier%22">M.-A. Pleier</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+Pleskot%22">V. Pleskot</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Plotnikova%22">E. Plotnikova</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Podberezko%22">P. Podberezko</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Poettgen%22">R. Poettgen</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Poggi%22">R. Poggi</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Poggioli%22">L. Poggioli</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+Pogrebnyak%22">I. Pogrebnyak</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Pohl%22">D. Pohl</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+Pokharel%22">I. Pokharel</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Polesello%22">G. Polesello</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Poley%22">A. Poley</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Policicchio%22">A. Policicchio</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Polifka%22">R. Polifka</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Polini%22">A. Polini</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+S%2E+Pollard%22">C. S. Pollard</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+Polychronakos%22">V. Polychronakos</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Ponomarenko%22">D. Ponomarenko</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Pontecorvo%22">L. Pontecorvo</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Popa%22">S. Popa</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+A%2E+Popeneciu%22">G. A. Popeneciu</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Portales%22">L. Portales</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+M%2E+Portillo+Quintero%22">D. M. Portillo Quintero</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Pospisil%22">S. Pospisil</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Potamianos%22">K. Potamianos</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+N%2E+Potrap%22">I. N. Potrap</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+J%2E+Potter%22">C. J. Potter</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+Potti%22">H. Potti</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Poulsen%22">T. Poulsen</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Poveda%22">J. Poveda</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+D%2E+Powell%22">T. D. Powell</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Pownall%22">G. Pownall</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+E%2E+Pozo+Astigarraga%22">M. E. Pozo Astigarraga</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Pralavorio%22">P. Pralavorio</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Prell%22">S. Prell</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Price%22">D. Price</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Primavera%22">M. Primavera</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Prince%22">S. Prince</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+L%2E+Proffitt%22">M. L. Proffitt</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+Proklova%22">N. Proklova</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Prokofiev%22">K. Prokofiev</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Prokoshin%22">F. Prokoshin</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Protopopescu%22">S. Protopopescu</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Proudfoot%22">J. Proudfoot</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Przybycien%22">M. Przybycien</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Pudzha%22">D. Pudzha</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Puri%22">A. Puri</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Puzo%22">P. Puzo</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Qian%22">J. Qian</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+Qin%22">Y. Qin</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Quadt%22">A. Quadt</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Queitsch-Maitland%22">M. Queitsch-Maitland</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Qureshi%22">A. Qureshi</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Racko%22">M. Racko</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Ragusa%22">F. Ragusa</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Rahal%22">G. Rahal</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+A%2E+Raine%22">J. A. Raine</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Rajagopalan%22">S. Rajagopalan</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Ramirez+Morales%22">A. Ramirez Morales</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Ran%22">K. Ran</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Rashid%22">T. Rashid</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Raspopov%22">S. Raspopov</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+M%2E+Rauch%22">D. M. Rauch</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Rauscher%22">F. Rauscher</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Rave%22">S. Rave</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Ravina%22">B. Ravina</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+Ravinovich%22">I. Ravinovich</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+H%2E+Rawling%22">J. H. Rawling</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Raymond%22">M. Raymond</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+L%2E+Read%22">A. L. Read</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+P%2E+Readioff%22">N. P. Readioff</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Reale%22">M. Reale</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+M%2E+Rebuzzi%22">D. M. Rebuzzi</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Redelbach%22">A. Redelbach</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Redlinger%22">G. Redlinger</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Reeves%22">K. Reeves</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Rehnisch%22">L. Rehnisch</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Reichert%22">J. Reichert</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Reikher%22">D. Reikher</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Reiss%22">A. Reiss</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Rej%22">A. Rej</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Rembser%22">C. Rembser</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Renda%22">M. Renda</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Rescigno%22">M. Rescigno</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Resconi%22">S. Resconi</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+D%2E+Resseguie%22">E. D. Resseguie</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Rettie%22">S. Rettie</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Reynolds%22">B. Reynolds</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Reynolds%22">E. Reynolds</searchLink><br /><searchLink fieldCode="AR" term="%22O%2E+L%2E+Rezanova%22">O. L. Rezanova</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Reznicek%22">P. Reznicek</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Ricci%22">E. Ricci</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Richter%22">R. Richter</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Richter%22">S. Richter</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Richter-Was%22">E. Richter-Was</searchLink><br /><searchLink fieldCode="AR" term="%22O%2E+Ricken%22">O. Ricken</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Ridel%22">M. Ridel</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Rieck%22">P. Rieck</searchLink><br /><searchLink fieldCode="AR" term="%22O%2E+Rifki%22">O. Rifki</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Rijssenbeek%22">M. Rijssenbeek</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Rimoldi%22">A. Rimoldi</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Rimoldi%22">M. Rimoldi</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Rinaldi%22">L. Rinaldi</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Ripellino%22">G. Ripellino</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+Riu%22">I. Riu</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+C%2E+Rivera+Vergara%22">J. C. Rivera Vergara</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Rizatdinova%22">F. Rizatdinova</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Rizvi%22">E. Rizvi</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Rizzi%22">C. Rizzi</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+T%2E+Roberts%22">R. T. Roberts</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+H%2E+Robertson%22">S. H. Robertson</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Robin%22">M. Robin</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Robinson%22">D. Robinson</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+E%2E+M%2E+Robinson%22">J. E. M. Robinson</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+M%2E+Robles+Gajardo%22">C. M. Robles Gajardo</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Robson%22">A. Robson</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Rocchi%22">A. Rocchi</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Rocco%22">E. Rocco</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Roda%22">C. Roda</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Rodriguez+Bosca%22">S. Rodriguez Bosca</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Rodriguez+Perez%22">A. Rodriguez Perez</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Rodriguez+Rodriguez%22">D. Rodriguez Rodriguez</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+M%2E+Rodríguez+Vera%22">A. M. Rodríguez Vera</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Roe%22">S. Roe</searchLink><br /><searchLink fieldCode="AR" term="%22O%2E+Røhne%22">O. Røhne</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Röhrig%22">R. Röhrig</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+A%2E+Rojas%22">R. A. Rojas</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+P%2E+A%2E+Roland%22">C. P. A. Roland</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Roloff%22">J. Roloff</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Romaniouk%22">A. Romaniouk</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Romano%22">M. Romano</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+Rompotis%22">N. Rompotis</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Ronzani%22">M. Ronzani</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Roos%22">L. Roos</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Rosati%22">S. Rosati</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Rosin%22">G. Rosin</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+J%2E+Rosser%22">B. J. Rosser</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Rossi%22">E. Rossi</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+P%2E+Rossi%22">L. P. Rossi</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Rossini%22">L. Rossini</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Rosten%22">R. Rosten</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Rotaru%22">M. Rotaru</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Rothberg%22">J. Rothberg</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Rousseau%22">D. Rousseau</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Rovelli%22">G. Rovelli</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Roy%22">A. Roy</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Roy%22">D. Roy</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Rozanov%22">A. Rozanov</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+Rozen%22">Y. Rozen</searchLink><br /><searchLink fieldCode="AR" term="%22X%2E+Ruan%22">X. Ruan</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Rühr%22">F. Rühr</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Ruiz-Martinez%22">A. Ruiz-Martinez</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Rummler%22">A. Rummler</searchLink><br /><searchLink fieldCode="AR" term="%22Z%2E+Rurikova%22">Z. Rurikova</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+A%2E+Rusakovich%22">N. A. Rusakovich</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+L%2E+Russell%22">H. L. Russell</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Rustige%22">L. Rustige</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+P%2E+Rutherfoord%22">J. P. Rutherfoord</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+M%2E+Rüttinger%22">E. M. Rüttinger</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Rybar%22">M. Rybar</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Rybkin%22">G. Rybkin</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+B%2E+Rye%22">E. B. Rye</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Ryzhov%22">A. Ryzhov</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+A%2E+Sabater+Iglesias%22">J. A. Sabater Iglesias</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Sabatini%22">P. Sabatini</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Sabato%22">G. Sabato</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Sacerdoti%22">S. Sacerdoti</searchLink><br /><searchLink fieldCode="AR" term="%22H%2EF-W%2E+Sadrozinski%22">H.F-W. Sadrozinski</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Sadykov%22">R. Sadykov</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Safai+Tehrani%22">F. Safai Tehrani</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Safarzadeh+Samani%22">B. Safarzadeh Samani</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Saha%22">P. Saha</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Saha%22">S. Saha</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Sahinsoy%22">M. Sahinsoy</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Sahu%22">A. Sahu</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Saimpert%22">M. Saimpert</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Saito%22">M. Saito</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Saito%22">T. Saito</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+Sakamoto%22">H. Sakamoto</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Sakharov%22">A. Sakharov</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Salamani%22">D. Salamani</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Salamanna%22">G. Salamanna</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+E%2E+Salazar+Loyola%22">J. E. Salazar Loyola</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Salnikov%22">A. Salnikov</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Salt%22">J. Salt</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Salvatore%22">D. Salvatore</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Salvatore%22">F. Salvatore</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Salvucci%22">A. Salvucci</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Salzburger%22">A. Salzburger</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Samarati%22">J. Samarati</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Sammel%22">D. Sammel</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Sampsonidis%22">D. Sampsonidis</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Sampsonidou%22">D. Sampsonidou</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Sánchez%22">J. Sánchez</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Sanchez+Pineda%22">A. Sanchez Pineda</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+Sandaker%22">H. Sandaker</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+O%2E+Sander%22">C. O. Sander</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+G%2E+Sanderswood%22">I. G. Sanderswood</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Sandhoff%22">M. Sandhoff</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Sandoval%22">C. Sandoval</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+P%2E+C%2E+Sankey%22">D. P. C. Sankey</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Sannino%22">M. Sannino</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+Sano%22">Y. Sano</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Sansoni%22">A. Sansoni</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Santoni%22">C. Santoni</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+Santos%22">H. Santos</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+N%2E+Santpur%22">S. N. Santpur</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Santra%22">A. Santra</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Sapronov%22">A. Sapronov</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+G%2E+Saraiva%22">J. G. Saraiva</searchLink><br /><searchLink fieldCode="AR" term="%22O%2E+Sasaki%22">O. Sasaki</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Sato%22">K. Sato</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Sauerburger%22">F. Sauerburger</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Sauvan%22">E. Sauvan</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Savard%22">P. Savard</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Sawada%22">R. Sawada</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Sawyer%22">C. Sawyer</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Sawyer%22">L. Sawyer</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Sbarra%22">C. Sbarra</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Sbrizzi%22">A. Sbrizzi</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Scanlon%22">T. Scanlon</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Schaarschmidt%22">J. Schaarschmidt</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Schacht%22">P. Schacht</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+M%2E+Schachtner%22">B. M. Schachtner</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Schaefer%22">D. Schaefer</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Schaefer%22">L. Schaefer</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Schaeffer%22">J. Schaeffer</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Schaepe%22">S. Schaepe</searchLink><br /><searchLink fieldCode="AR" term="%22U%2E+Schäfer%22">U. Schäfer</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+C%2E+Schaffer%22">A. C. Schaffer</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Schaile%22">D. Schaile</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+D%2E+Schamberger%22">R. D. Schamberger</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+Scharmberg%22">N. Scharmberg</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+A%2E+Schegelsky%22">V. A. Schegelsky</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Scheirich%22">D. Scheirich</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Schenck%22">F. Schenck</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Schernau%22">M. Schernau</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Schiavi%22">C. Schiavi</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Schier%22">S. Schier</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+K%2E+Schildgen%22">L. K. Schildgen</searchLink><br /><searchLink fieldCode="AR" term="%22Z%2E+M%2E+Schillaci%22">Z. M. Schillaci</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+J%2E+Schioppa%22">E. J. Schioppa</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Schioppa%22">M. Schioppa</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+E%2E+Schleicher%22">K. E. Schleicher</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Schlenker%22">S. Schlenker</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+R%2E+Schmidt-Sommerfeld%22">K. R. Schmidt-Sommerfeld</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Schmieden%22">K. Schmieden</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Schmitt%22">C. Schmitt</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Schmitt%22">S. Schmitt</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Schmitz%22">S. Schmitz</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+C%2E+Schmoeckel%22">J. C. Schmoeckel</searchLink><br /><searchLink fieldCode="AR" term="%22U%2E+Schnoor%22">U. Schnoor</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Schoeffel%22">L. Schoeffel</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Schoening%22">A. Schoening</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+G%2E+Scholer%22">P. G. Scholer</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Schopf%22">E. Schopf</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Schott%22">M. Schott</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+F%2E+P%2E+Schouwenberg%22">J. F. P. Schouwenberg</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Schovancova%22">J. Schovancova</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Schramm%22">S. Schramm</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Schroeder%22">F. Schroeder</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Schulte%22">A. Schulte</searchLink><br /><searchLink fieldCode="AR" term="%22H-C%2E+Schultz-Coulon%22">H-C. Schultz-Coulon</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Schumacher%22">M. Schumacher</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+A%2E+Schumm%22">B. A. Schumm</searchLink><br /><searchLink fieldCode="AR" term="%22Ph%2E+Schune%22">Ph. Schune</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Schwartzman%22">A. Schwartzman</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+A%2E+Schwarz%22">T. A. Schwarz</searchLink><br /><searchLink fieldCode="AR" term="%22Ph%2E+Schwemling%22">Ph. Schwemling</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Schwienhorst%22">R. Schwienhorst</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Sciandra%22">A. Sciandra</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Sciolla%22">G. Sciolla</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Scodeggio%22">M. Scodeggio</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Scornajenghi%22">M. Scornajenghi</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Scuri%22">F. Scuri</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Scutti%22">F. Scutti</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+M%2E+Scyboz%22">L. M. Scyboz</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+D%2E+Sebastiani%22">C. D. Sebastiani</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Seema%22">P. Seema</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+C%2E+Seidel%22">S. C. Seidel</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Seiden%22">A. Seiden</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+D%2E+Seidlitz%22">B. D. Seidlitz</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Seiss%22">T. Seiss</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+M%2E+Seixas%22">J. M. Seixas</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Sekhniaidze%22">G. Sekhniaidze</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Sekhon%22">K. Sekhon</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+J%2E+Sekula%22">S. J. Sekula</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+Semprini-Cesari%22">N. Semprini-Cesari</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Sen%22">S. Sen</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Serfon%22">C. Serfon</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Serin%22">L. Serin</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Serkin%22">L. Serkin</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Sessa%22">M. Sessa</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+Severini%22">H. Severini</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Sevova%22">S. Sevova</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Šfiligoj%22">T. Šfiligoj</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Sforza%22">F. Sforza</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Sfyrla%22">A. Sfyrla</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Shabalina%22">E. Shabalina</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+D%2E+Shahinian%22">J. D. Shahinian</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+W%2E+Shaikh%22">N. W. Shaikh</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Shaked+Renous%22">D. Shaked Renous</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Y%2E+Shan%22">L. Y. Shan</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+T%2E+Shank%22">J. T. Shank</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Shapiro%22">M. Shapiro</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Sharma%22">A. Sharma</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+S%2E+Sharma%22">A. S. Sharma</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+B%2E+Shatalov%22">P. B. Shatalov</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Shaw%22">K. Shaw</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+M%2E+Shaw%22">S. M. Shaw</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Shehade%22">M. Shehade</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+Shen%22">Y. Shen</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+D%2E+Sherman%22">A. D. Sherman</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Sherwood%22">P. Sherwood</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Shi%22">L. Shi</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Shimizu%22">S. Shimizu</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+O%2E+Shimmin%22">C. O. Shimmin</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+Shimogama%22">Y. Shimogama</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Shimojima%22">M. Shimojima</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+P%2E+J%2E+Shipsey%22">I. P. J. Shipsey</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Shirabe%22">S. Shirabe</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Shiyakova%22">M. Shiyakova</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Shlomi%22">J. Shlomi</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Shmeleva%22">A. Shmeleva</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+J%2E+Shochet%22">M. J. Shochet</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Shojaii%22">J. Shojaii</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+R%2E+Shope%22">D. R. Shope</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Shrestha%22">S. Shrestha</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+M%2E+Shrif%22">E. M. Shrif</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Shulga%22">E. Shulga</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Sicho%22">P. Sicho</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+M%2E+Sickles%22">A. M. Sickles</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+E%2E+Sidebo%22">P. E. Sidebo</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Sideras+Haddad%22">E. Sideras Haddad</searchLink><br /><searchLink fieldCode="AR" term="%22O%2E+Sidiropoulou%22">O. Sidiropoulou</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Sidoti%22">A. Sidoti</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Siegert%22">F. Siegert</searchLink><br /><searchLink fieldCode="AR" term="%22Dj%2E+Sijacki%22">Dj. Sijacki</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Jr%2E+Silva%22">M. Jr. Silva</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+V%2E+Silva+Oliveira%22">M. V. Silva Oliveira</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+B%2E+Silverstein%22">S. B. Silverstein</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Simion%22">S. Simion</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Simoniello%22">R. Simoniello</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Simsek%22">S. Simsek</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Sinervo%22">P. Sinervo</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+Sinetckii%22">V. Sinetckii</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+B%2E+Sinev%22">N. B. Sinev</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Singh%22">S. Singh</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Sioli%22">M. Sioli</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+Siral%22">I. Siral</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Yu%2E+Sivoklokov%22">S. Yu. Sivoklokov</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Sjölin%22">J. Sjölin</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Skorda%22">E. Skorda</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Skubic%22">P. Skubic</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Slawinska%22">M. Slawinska</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Sliwa%22">K. Sliwa</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Slovak%22">R. Slovak</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+Smakhtin%22">V. Smakhtin</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+H%2E+Smart%22">B. H. Smart</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Smiesko%22">J. Smiesko</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+Smirnov%22">N. Smirnov</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Yu%2E+Smirnov%22">S. Yu. Smirnov</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+Smirnov%22">Y. Smirnov</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+N%2E+Smirnova%22">L. N. Smirnova</searchLink><br /><searchLink fieldCode="AR" term="%22O%2E+Smirnova%22">O. Smirnova</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+W%2E+Smith%22">J. W. Smith</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Smizanska%22">M. Smizanska</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Smolek%22">K. Smolek</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Smykiewicz%22">A. Smykiewicz</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+A%2E+Snesarev%22">A. A. Snesarev</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+L%2E+Snoek%22">H. L. Snoek</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+M%2E+Snyder%22">I. M. Snyder</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Snyder%22">S. Snyder</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Sobie%22">R. Sobie</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Soffer%22">A. Soffer</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Søgaard%22">A. Søgaard</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Sohns%22">F. Sohns</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+A%2E+Solans+Sanchez%22">C. A. Solans Sanchez</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Yu%2E+Soldatov%22">E. Yu. Soldatov</searchLink><br /><searchLink fieldCode="AR" term="%22U%2E+Soldevila%22">U. Soldevila</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+A%2E+Solodkov%22">A. A. Solodkov</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Soloshenko%22">A. Soloshenko</searchLink><br /><searchLink fieldCode="AR" term="%22O%2E+V%2E+Solovyanov%22">O. V. Solovyanov</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+Solovyev%22">V. Solovyev</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Sommer%22">P. Sommer</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+Son%22">H. Son</searchLink><br /><searchLink fieldCode="AR" term="%22W%2E+Song%22">W. Song</searchLink><br /><searchLink fieldCode="AR" term="%22W%2E+Y%2E+Song%22">W. Y. Song</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Sopczak%22">A. Sopczak</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+L%2E+Sopio%22">A. L. Sopio</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Sopkova%22">F. Sopkova</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+L%2E+Sotiropoulou%22">C. L. Sotiropoulou</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Sottocornola%22">S. Sottocornola</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Soualah%22">R. Soualah</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+M%2E+Soukharev%22">A. M. Soukharev</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+South%22">D. South</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Spagnolo%22">S. Spagnolo</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Spalla%22">M. Spalla</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Spangenberg%22">M. Spangenberg</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Spanò%22">F. Spanò</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Sperlich%22">D. Sperlich</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+M%2E+Spieker%22">T. M. Spieker</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Spighi%22">R. Spighi</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Spigo%22">G. Spigo</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Spina%22">M. Spina</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+P%2E+Spiteri%22">D. P. Spiteri</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Spousta%22">M. Spousta</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Stabile%22">A. Stabile</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+L%2E+Stamas%22">B. L. Stamas</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Stamen%22">R. Stamen</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Stamenkovic%22">M. Stamenkovic</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Stanecka%22">E. Stanecka</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Stanislaus%22">B. Stanislaus</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+M%2E+Stanitzki%22">M. M. Stanitzki</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Stankaityte%22">M. Stankaityte</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Stapf%22">B. Stapf</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+A%2E+Starchenko%22">E. A. Starchenko</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+H%2E+Stark%22">G. H. Stark</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Stark%22">J. Stark</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+H%2E+Stark%22">S. H. Stark</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Staroba%22">P. Staroba</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Starovoitov%22">P. Starovoitov</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Stärz%22">S. Stärz</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Staszewski%22">R. Staszewski</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Stavropoulos%22">G. Stavropoulos</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Stegler%22">M. Stegler</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Steinberg%22">P. Steinberg</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+L%2E+Steinhebel%22">A. L. Steinhebel</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Stelzer%22">B. Stelzer</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+J%2E+Stelzer%22">H. J. Stelzer</searchLink><br /><searchLink fieldCode="AR" term="%22O%2E+Stelzer-Chilton%22">O. Stelzer-Chilton</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+Stenzel%22">H. Stenzel</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+J%2E+Stevenson%22">T. J. Stevenson</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+A%2E+Stewart%22">G. A. Stewart</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+C%2E+Stockton%22">M. C. Stockton</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Stoicea%22">G. Stoicea</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Stolarski%22">M. Stolarski</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Stonjek%22">S. Stonjek</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Straessner%22">A. Straessner</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Strandberg%22">J. Strandberg</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Strandberg%22">S. Strandberg</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Strauss%22">M. Strauss</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Strizenec%22">P. Strizenec</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Ströhmer%22">R. Ströhmer</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+M%2E+Strom%22">D. M. Strom</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Stroynowski%22">R. Stroynowski</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Strubig%22">A. Strubig</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+A%2E+Stucci%22">S. A. Stucci</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Stugu%22">B. Stugu</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Stupak%22">J. Stupak</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+A%2E+Styles%22">N. A. Styles</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Su%22">D. Su</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Suchek%22">S. Suchek</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+V%2E+Sulin%22">V. V. Sulin</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+J%2E+Sullivan%22">M. J. Sullivan</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+M%2E+S%2E+Sultan%22">D. M. S. Sultan</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Sultansoy%22">S. Sultansoy</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Sumida%22">T. Sumida</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Sun%22">S. Sun</searchLink><br /><searchLink fieldCode="AR" term="%22X%2E+Sun%22">X. Sun</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Suruliz%22">K. Suruliz</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+J%2E+E%2E+Suster%22">C. J. E. Suster</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+R%2E+Sutton%22">M. R. Sutton</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Suzuki%22">S. Suzuki</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Svatos%22">M. Svatos</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Swiatlowski%22">M. Swiatlowski</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+P%2E+Swift%22">S. P. Swift</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Swirski%22">T. Swirski</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Sydorenko%22">A. Sydorenko</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+Sykora%22">I. Sykora</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Sykora%22">M. Sykora</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Sykora%22">T. Sykora</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Ta%22">D. Ta</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Tackmann%22">K. Tackmann</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Taenzer%22">J. Taenzer</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Taffard%22">A. Taffard</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Tafirout%22">R. Tafirout</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+Takai%22">H. Takai</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Takashima%22">R. Takashima</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Takeda%22">K. Takeda</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Takeshita%22">T. Takeshita</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+P%2E+Takeva%22">E. P. Takeva</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+Takubo%22">Y. Takubo</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Talby%22">M. Talby</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+A%2E+Talyshev%22">A. A. Talyshev</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+M%2E+Tamir%22">N. M. Tamir</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Tanaka%22">J. Tanaka</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Tanaka%22">M. Tanaka</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Tanaka%22">R. Tanaka</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Tapia+Araya%22">S. Tapia Araya</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Tapprogge%22">S. Tapprogge</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Tarek+Abouelfadl+Mohamed%22">A. Tarek Abouelfadl Mohamed</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Tarem%22">S. Tarem</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Tariq%22">K. Tariq</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Tarna%22">G. Tarna</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+F%2E+Tartarelli%22">G. F. Tartarelli</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Tas%22">P. Tas</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Tasevsky%22">M. Tasevsky</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Tashiro%22">T. Tashiro</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Tassi%22">E. Tassi</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Tavares+Delgado%22">A. Tavares Delgado</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+Tayalati%22">Y. Tayalati</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+J%2E+Taylor%22">A. J. Taylor</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+N%2E+Taylor%22">G. N. Taylor</searchLink><br /><searchLink fieldCode="AR" term="%22W%2E+Taylor%22">W. Taylor</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+S%2E+Tee%22">A. S. Tee</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Teixeira+De+Lima%22">R. Teixeira De Lima</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Teixeira-Dias%22">P. Teixeira-Dias</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+Ten+Kate%22">H. Ten Kate</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+J%2E+Teoh%22">J. J. Teoh</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Terada%22">S. Terada</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Terashi%22">K. Terashi</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Terron%22">J. Terron</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Terzo%22">S. Terzo</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Testa%22">M. Testa</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+J%2E+Teuscher%22">R. J. Teuscher</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+J%2E+Thais%22">S. J. Thais</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Theveneaux-Pelzer%22">T. Theveneaux-Pelzer</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Thiele%22">F. Thiele</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+W%2E+Thomas%22">D. W. Thomas</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+O%2E+Thomas%22">J. O. Thomas</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+P%2E+Thomas%22">J. P. Thomas</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+S%2E+Thompson%22">A. S. Thompson</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+D%2E+Thompson%22">P. D. Thompson</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+A%2E+Thomsen%22">L. A. Thomsen</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Thomson%22">E. Thomson</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+J%2E+Thorpe%22">E. J. Thorpe</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+E%2E+Ticse+Torres%22">R. E. Ticse Torres</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+O%2E+Tikhomirov%22">V. O. Tikhomirov</searchLink><br /><searchLink fieldCode="AR" term="%22Yu%2E+A%2E+Tikhonov%22">Yu. A. Tikhonov</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Timoshenko%22">S. Timoshenko</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Tipton%22">P. Tipton</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Tisserant%22">S. Tisserant</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Todome%22">K. Todome</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Todorova-Nova%22">S. Todorova-Nova</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Todt%22">S. Todt</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Tojo%22">J. Tojo</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Tokár%22">S. Tokár</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Tokushuku%22">K. Tokushuku</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Tolley%22">E. Tolley</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+G%2E+Tomiwa%22">K. G. Tomiwa</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Tomoto%22">M. Tomoto</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Tompkins%22">L. Tompkins</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Tong%22">B. Tong</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Tornambe%22">P. Tornambe</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Torrence%22">E. Torrence</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+Torres%22">H. Torres</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Torró+Pastor%22">E. Torró Pastor</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Tosciri%22">C. Tosciri</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Toth%22">J. Toth</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+R%2E+Tovey%22">D. R. Tovey</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Traeet%22">A. Traeet</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+J%2E+Treado%22">C. J. Treado</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Trefzger%22">T. Trefzger</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Tresoldi%22">F. Tresoldi</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Tricoli%22">A. Tricoli</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+M%2E+Trigger%22">I. M. Trigger</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Trincaz-Duvoid%22">S. Trincaz-Duvoid</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+T%2E+Trischuk%22">D. T. Trischuk</searchLink><br /><searchLink fieldCode="AR" term="%22W%2E+Trischuk%22">W. Trischuk</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Trocmé%22">B. Trocmé</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Trofymov%22">A. Trofymov</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Troncon%22">C. Troncon</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Trovatelli%22">M. Trovatelli</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Trovato%22">F. Trovato</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Truong%22">L. Truong</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Trzebinski%22">M. Trzebinski</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Trzupek%22">A. Trzupek</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Tsai%22">F. Tsai</searchLink><br /><searchLink fieldCode="AR" term="%22J%2EC-L%2E+Tseng%22">J.C-L. Tseng</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+V%2E+Tsiareshka%22">P. V. Tsiareshka</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Tsirigotis%22">A. Tsirigotis</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+Tsiskaridze%22">V. Tsiskaridze</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+G%2E+Tskhadadze%22">E. G. Tskhadadze</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Tsopoulou%22">M. Tsopoulou</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+I%2E+Tsukerman%22">I. I. Tsukerman</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+Tsulaia%22">V. Tsulaia</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Tsuno%22">S. Tsuno</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Tsybychev%22">D. Tsybychev</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+Tu%22">Y. Tu</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Tudorache%22">A. Tudorache</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+Tudorache%22">V. Tudorache</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+T%2E+Tulbure%22">T. T. Tulbure</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+N%2E+Tuna%22">A. N. Tuna</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Turchikhin%22">S. Turchikhin</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Turgeman%22">D. Turgeman</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+Turk+Cakir%22">I. Turk Cakir</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+J%2E+Turner%22">R. J. Turner</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+T%2E+Turra%22">R. T. Turra</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+M%2E+Tuts%22">P. M. Tuts</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Tzamarias%22">S. Tzamarias</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Tzovara%22">E. Tzovara</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Ucchielli%22">G. Ucchielli</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Uchida%22">K. Uchida</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+Ueda%22">I. Ueda</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Ukegawa%22">F. Ukegawa</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Unal%22">G. Unal</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Undrus%22">A. Undrus</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Unel%22">G. Unel</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+C%2E+Ungaro%22">F. C. Ungaro</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+Unno%22">Y. Unno</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Uno%22">K. Uno</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Urban%22">J. Urban</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Urquijo%22">P. Urquijo</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Usai%22">G. Usai</searchLink><br /><searchLink fieldCode="AR" term="%22Z%2E+Uysal%22">Z. Uysal</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+Vacek%22">V. Vacek</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+Vachon%22">B. Vachon</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+O%2E+H%2E+Vadla%22">K. O. H. Vadla</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Vaidya%22">A. Vaidya</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Valderanis%22">C. Valderanis</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Valdes+Santurio%22">E. Valdes Santurio</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Valente%22">M. Valente</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Valentinetti%22">S. Valentinetti</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Valero%22">A. Valero</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Valéry%22">L. Valéry</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+A%2E+Vallance%22">R. A. Vallance</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Vallier%22">A. Vallier</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+A%2E+Valls+Ferrer%22">J. A. Valls Ferrer</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+R%2E+Van+Daalen%22">T. R. Van Daalen</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Van+Gemmeren%22">P. Van Gemmeren</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+Van+Vulpen%22">I. Van Vulpen</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Vanadia%22">M. Vanadia</searchLink><br /><searchLink fieldCode="AR" term="%22W%2E+Vandelli%22">W. Vandelli</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Vandenbroucke%22">M. Vandenbroucke</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+R%2E+Vandewall%22">E. R. Vandewall</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Vaniachine%22">A. Vaniachine</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Vannicola%22">D. Vannicola</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Vari%22">R. Vari</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+W%2E+Varnes%22">E. W. Varnes</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Varni%22">C. Varni</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Varol%22">T. Varol</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Varouchas%22">D. Varouchas</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+E%2E+Varvell%22">K. E. Varvell</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+E%2E+Vasile%22">M. E. Vasile</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+A%2E+Vasquez%22">G. A. Vasquez</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Vazeille%22">F. Vazeille</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Vazquez+Furelos%22">D. Vazquez Furelos</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Vazquez+Schroeder%22">T. Vazquez Schroeder</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Veatch%22">J. Veatch</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+Vecchio%22">V. Vecchio</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+J%2E+Veen%22">M. J. Veen</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+M%2E+Veloce%22">L. M. Veloce</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Veloso%22">F. Veloso</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Veneziano%22">S. Veneziano</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Ventura%22">A. Ventura</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+Venturi%22">N. Venturi</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Verbytskyi%22">A. Verbytskyi</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+Vercesi%22">V. Vercesi</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Verducci%22">M. Verducci</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+M%2E+Vergel+Infante%22">C. M. Vergel Infante</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Vergis%22">C. Vergis</searchLink><br /><searchLink fieldCode="AR" term="%22W%2E+Verkerke%22">W. Verkerke</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+T%2E+Vermeulen%22">A. T. Vermeulen</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+C%2E+Vermeulen%22">J. C. Vermeulen</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+C%2E+Vetterli%22">M. C. Vetterli</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+Viaux+Maira%22">N. Viaux Maira</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Vicente+Barreto+Pinto%22">M. Vicente Barreto Pinto</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Vickey%22">T. Vickey</searchLink><br /><searchLink fieldCode="AR" term="%22O%2E+E%2E+Vickey+Boeriu%22">O. E. Vickey Boeriu</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+H%2E+A%2E+Viehhauser%22">G. H. A. Viehhauser</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+Vigani%22">L. Vigani</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Villa%22">M. Villa</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Villaplana+Perez%22">M. Villaplana Perez</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Vilucchi%22">E. Vilucchi</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+G%2E+Vincter%22">M. G. Vincter</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+S%2E+Virdee%22">G. S. Virdee</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Vishwakarma%22">A. Vishwakarma</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Vittori%22">C. Vittori</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+Vivarelli%22">I. Vivarelli</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Vogel%22">M. Vogel</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Vokac%22">P. Vokac</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+E%2E+von+Buddenbrock%22">S. E. von Buddenbrock</searchLink><br /><searchLink fieldCode="AR" term="%22E%2E+Von+Toerne%22">E. Von Toerne</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+Vorobel%22">V. Vorobel</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Vorobev%22">K. Vorobev</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Vos%22">M. Vos</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+H%2E+Vossebeld%22">J. H. Vossebeld</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Vozak%22">M. Vozak</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+Vranjes%22">N. Vranjes</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Vranjes+Milosavljevic%22">M. Vranjes Milosavljevic</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+Vrba%22">V. Vrba</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Vreeswijk%22">M. Vreeswijk</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Vuillermet%22">R. Vuillermet</searchLink><br /><searchLink fieldCode="AR" term="%22I%2E+Vukotic%22">I. Vukotic</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Wagner%22">P. Wagner</searchLink><br /><searchLink fieldCode="AR" term="%22W%2E+Wagner%22">W. Wagner</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Wagner-Kuhr%22">J. Wagner-Kuhr</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Wahdan%22">S. Wahdan</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+Wahlberg%22">H. Wahlberg</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+M%2E+Walbrecht%22">V. M. Walbrecht</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Walder%22">J. Walder</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Walker%22">R. Walker</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+D%2E+Walker%22">S. D. Walker</searchLink><br /><searchLink fieldCode="AR" term="%22W%2E+Walkowiak%22">W. Walkowiak</searchLink><br /><searchLink fieldCode="AR" term="%22V%2E+Wallangen%22">V. Wallangen</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+M%2E+Wang%22">A. M. Wang</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Wang%22">C. Wang</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Wang%22">F. Wang</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+Wang%22">H. Wang</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Wang%22">J. Wang</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+Wang%22">P. Wang</searchLink><br /><searchLink fieldCode="AR" term="%22Q%2E+Wang%22">Q. Wang</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E-J%2E+Wang%22">R.-J. Wang</searchLink><br /><searchLink fieldCode="AR" term="%22R%2E+Wang%22">R. Wang</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+M%2E+Wang%22">S. M. Wang</searchLink><br /><searchLink fieldCode="AR" term="%22W%2E+T%2E+Wang%22">W. T. Wang</searchLink><br /><searchLink fieldCode="AR" term="%22W%2E+Wang%22">W. Wang</searchLink><br /><searchLink fieldCode="AR" term="%22W%2E+X%2E+Wang%22">W. X. Wang</searchLink><br /><searchLink fieldCode="AR" term="%22Y%2E+Wang%22">Y. Wang</searchLink><br /><searchLink fieldCode="AR" term="%22Z%2E+Wang%22">Z. Wang</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Wanotayaroj%22">C. Wanotayaroj</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Warburton%22">A. Warburton</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+P%2E+Ward%22">C. P. Ward</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+R%2E+Wardrope%22">D. R. Wardrope</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+Warrack%22">N. Warrack</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+Washbrook%22">A. Washbrook</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+T%2E+Watson%22">A. T. Watson</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+F%2E+Watson%22">M. F. Watson</searchLink><br /><searchLink fieldCode="AR" term="%22G%2E+Watts%22">G. Watts</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+M%2E+Waugh%22">B. M. Waugh</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+F%2E+Webb%22">A. F. Webb</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Webb%22">S. Webb</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Weber%22">C. Weber</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+S%2E+Weber%22">M. S. Weber</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+A%2E+Weber%22">S. A. Weber</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+M%2E+Weber%22">S. M. Weber</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+R%2E+Weidberg%22">A. R. Weidberg</searchLink><br /><searchLink fieldCode="AR" term="%22J%2E+Weingarten%22">J. Weingarten</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Weirich%22">M. Weirich</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Weiser%22">C. Weiser</searchLink><br /><searchLink fieldCode="AR" term="%22P%2E+S%2E+Wells%22">P. S. Wells</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Wenaus%22">T. Wenaus</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+Wengler%22">T. Wengler</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Wenig%22">S. Wenig</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+Wermes%22">N. Wermes</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+D%2E+Werner%22">M. D. Werner</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Wessels%22">M. Wessels</searchLink><br /><searchLink fieldCode="AR" term="%22T%2E+D%2E+Weston%22">T. D. Weston</searchLink><br /><searchLink fieldCode="AR" term="%22K%2E+Whalen%22">K. Whalen</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+L%2E+Whallon%22">N. L. Whallon</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+M%2E+Wharton%22">A. M. Wharton</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+S%2E+White%22">A. S. White</searchLink><br /><searchLink fieldCode="AR" term="%22A%2E+White%22">A. White</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+J%2E+White%22">M. J. White</searchLink><br /><searchLink fieldCode="AR" term="%22D%2E+Whiteson%22">D. Whiteson</searchLink><br /><searchLink fieldCode="AR" term="%22B%2E+W%2E+Whitmore%22">B. W. Whitmore</searchLink><br /><searchLink fieldCode="AR" term="%22W%2E+Wiedenmann%22">W. Wiedenmann</searchLink><br /><searchLink fieldCode="AR" term="%22M%2E+Wielers%22">M. Wielers</searchLink><br /><searchLink fieldCode="AR" term="%22N%2E+Wieseotte%22">N. Wieseotte</searchLink><br /><searchLink fieldCode="AR" term="%22C%2E+Wiglesworth%22">C. Wiglesworth</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+A%2E+M%2E+Wiik-Fuchs%22">L. A. M. Wiik-Fuchs</searchLink><br /><searchLink fieldCode="AR" term="%22F%2E+Wilk%22">F. Wilk</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+G%2E+Wilkens%22">H. G. Wilkens</searchLink><br /><searchLink fieldCode="AR" term="%22L%2E+J%2E+Wilkins%22">L. J. Wilkins</searchLink><br /><searchLink fieldCode="AR" term="%22H%2E+H%2E+Williams%22">H. H. Williams</searchLink><br /><searchLink fieldCode="AR" term="%22S%2E+Williams%22">S. 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– Name: TitleSource
  Label: Source
  Group: Src
  Data: European Physical Journal C: Particles and Fields, Vol 80, Iss 6, Pp 1-70 (2020)
– Name: Publisher
  Label: Publisher Information
  Group: PubInfo
  Data: SpringerOpen, 2020.
– Name: DatePubCY
  Label: Publication Year
  Group: Date
  Data: 2020
– Name: Subset
  Label: Collection
  Group: HoldingsInfo
  Data: LCC:Astrophysics<br />LCC:Nuclear and particle physics. Atomic energy. Radioactivity
– Name: Subject
  Label: Subject Terms
  Group: Su
  Data: <searchLink fieldCode="DE" term="%22Astrophysics%22">Astrophysics</searchLink><br /><searchLink fieldCode="DE" term="%22QB460-466%22">QB460-466</searchLink><br /><searchLink fieldCode="DE" term="%22Nuclear+and+particle+physics%2E+Atomic+energy%2E+Radioactivity%22">Nuclear and particle physics. Atomic energy. Radioactivity</searchLink><br /><searchLink fieldCode="DE" term="%22QC770-798%22">QC770-798</searchLink>
– Name: Abstract
  Label: Description
  Group: Ab
  Data: Abstract The inclusive top quark pair ($$t\bar{t}$$ tt¯ ) production cross-section $$\sigma _{t\bar{t}}$$ σtt¯ has been measured in proton–proton collisions at $$\sqrt{s}=13\,\text {TeV}$$ s=13TeV , using 36.1 fb$$^{-1}$$ -1 of data collected in 2015–2016 by the ATLAS experiment at the LHC. Using events with an opposite-charge $$e\mu $$ eμ pair and b-tagged jets, the cross-section is measured to be: $$\begin{aligned} \sigma _{t\bar{t}} = 826.4 \pm 3.6\,\mathrm {(stat)}\ \pm 11.5\,\mathrm {(syst)}\ \pm 15.7\,\mathrm {(lumi)}\ \pm 1.9\,\mathrm {(beam)}\,\mathrm {pb}, \end{aligned}$$ σtt¯=826.4±3.6(stat)±11.5(syst)±15.7(lumi)±1.9(beam)pb, where the uncertainties reflect the limited size of the data sample, experimental and theoretical systematic effects, the integrated luminosity, and the LHC beam energy, giving a total uncertainty of 2.4%. The result is consistent with theoretical QCD calculations at next-to-next-to-leading order. It is used to determine the top quark pole mass via the dependence of the predicted cross-section on $$m_t^{\mathrm{pole}}$$ mtpole , giving $$m_t^{\mathrm{pole}}=173.1^{+2.0}_{-2.1}\,\text {GeV}$$ mtpole=173.1-2.1+2.0GeV . It is also combined with measurements at $$\sqrt{s}=7\,\text {TeV}$$ s=7TeV and $$\sqrt{s}=8\,\text {TeV}$$ s=8TeV to derive ratios and double ratios of $$t\bar{t}$$ tt¯ and Z cross-sections at different energies. The same event sample is used to measure absolute and normalised differential cross-sections as functions of single-lepton and dilepton kinematic variables, and the results are compared with predictions from various Monte Carlo event generators.
– Name: TypeDocument
  Label: Document Type
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  Data: article
– Name: Format
  Label: File Description
  Group: SrcInfo
  Data: electronic resource
– Name: Language
  Label: Language
  Group: Lang
  Data: English
– Name: ISSN
  Label: ISSN
  Group: ISSN
  Data: 1434-6044<br />1434-6052
– Name: NoteTitleSource
  Label: Relation
  Group: SrcInfo
  Data: http://link.springer.com/article/10.1140/epjc/s10052-020-7907-9; https://doaj.org/toc/1434-6044; https://doaj.org/toc/1434-6052
– Name: DOI
  Label: DOI
  Group: ID
  Data: 10.1140/epjc/s10052-020-7907-9
– Name: URL
  Label: Access URL
  Group: URL
  Data: <link linkTarget="URL" linkTerm="https://doaj.org/article/b75d565816a64c408609a2f7ae9e8643" linkWindow="_blank">https://doaj.org/article/b75d565816a64c408609a2f7ae9e8643</link>
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  Data: edsdoj.b75d565816a64c408609a2f7ae9e8643
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        Value: 10.1140/epjc/s10052-020-7907-9
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      – Text: English
    PhysicalDescription:
      Pagination:
        PageCount: 70
        StartPage: 1
    Subjects:
      – SubjectFull: Astrophysics
        Type: general
      – SubjectFull: QB460-466
        Type: general
      – SubjectFull: Nuclear and particle physics. Atomic energy. Radioactivity
        Type: general
      – SubjectFull: QC770-798
        Type: general
    Titles:
      – TitleFull: Measurement of the $$t\bar{t}$$ tt¯ production cross-section and lepton differential distributions in $$e\mu $$ eμ dilepton events from pp collisions at $$\sqrt{s}=13\,\text {TeV}$$ s=13TeV with the ATLAS detector
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            NameFull: M. J. Basso
      – PersonEntity:
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            NameFull: R. L. Bates
      – PersonEntity:
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            NameFull: S. Batlamous
      – PersonEntity:
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            NameFull: J. R. Batley
      – PersonEntity:
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            NameFull: B. Batool
      – PersonEntity:
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      – PersonEntity:
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            NameFull: M. Bauce
      – PersonEntity:
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            NameFull: F. Bauer
      – PersonEntity:
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            NameFull: K. T. Bauer
      – PersonEntity:
          Name:
            NameFull: H. S. Bawa
      – PersonEntity:
          Name:
            NameFull: J. B. Beacham
      – PersonEntity:
          Name:
            NameFull: T. Beau
      – PersonEntity:
          Name:
            NameFull: P. H. Beauchemin
      – PersonEntity:
          Name:
            NameFull: F. Becherer
      – PersonEntity:
          Name:
            NameFull: P. Bechtle
      – PersonEntity:
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            NameFull: H. C. Beck
      – PersonEntity:
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            NameFull: H. P. Beck
      – PersonEntity:
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            NameFull: K. Becker
      – PersonEntity:
          Name:
            NameFull: M. Becker
      – PersonEntity:
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            NameFull: C. Becot
      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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            NameFull: C. P. Bee
      – PersonEntity:
          Name:
            NameFull: T. A. Beermann
      – PersonEntity:
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            NameFull: M. Begalli
      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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            NameFull: G. Bella
      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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            NameFull: P. Bellos
      – PersonEntity:
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      – PersonEntity:
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            NameFull: K. Belotskiy
      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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            NameFull: N. Benekos
      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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            NameFull: S. Bentvelsen
      – PersonEntity:
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      – PersonEntity:
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            NameFull: M. Beretta
      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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            NameFull: G. Brandt
      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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            NameFull: R. Brock
      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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            NameFull: E. Brost
      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
          Name:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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            NameFull: T. Dreyer
      – PersonEntity:
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            NameFull: A. S. Drobac
      – PersonEntity:
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            NameFull: D. Du
      – PersonEntity:
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      – PersonEntity:
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            NameFull: F. Dubinin
      – PersonEntity:
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            NameFull: M. Dubovsky
      – PersonEntity:
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            NameFull: A. Dubreuil
      – PersonEntity:
          Name:
            NameFull: E. Duchovni
      – PersonEntity:
          Name:
            NameFull: G. Duckeck
      – PersonEntity:
          Name:
            NameFull: A. Ducourthial
      – PersonEntity:
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            NameFull: O. A. Ducu
      – PersonEntity:
          Name:
            NameFull: D. Duda
      – PersonEntity:
          Name:
            NameFull: A. Dudarev
      – PersonEntity:
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            NameFull: A. C. Dudder
      – PersonEntity:
          Name:
            NameFull: E. M. Duffield
      – PersonEntity:
          Name:
            NameFull: L. Duflot
      – PersonEntity:
          Name:
            NameFull: M. Dührssen
      – PersonEntity:
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            NameFull: C. Dülsen
      – PersonEntity:
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            NameFull: M. Dumancic
      – PersonEntity:
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            NameFull: A. E. Dumitriu
      – PersonEntity:
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      – PersonEntity:
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            NameFull: M. Dunford
      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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            NameFull: M. Düren
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      – PersonEntity:
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            NameFull: D. Duschinger
      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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            NameFull: G. I. Dyckes
      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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            NameFull: T. Eifert
      – PersonEntity:
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            NameFull: G. Eigen
      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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            NameFull: M. Ellert
      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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            NameFull: O. L. Fedin
      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
          Name:
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      – PersonEntity:
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      – PersonEntity:
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            NameFull: K. Hanagaki
      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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            NameFull: G. Introzzi
      – PersonEntity:
          Name:
            NameFull: M. Iodice
      – PersonEntity:
          Name:
            NameFull: K. Iordanidou
      – PersonEntity:
          Name:
            NameFull: V. Ippolito
      – PersonEntity:
          Name:
            NameFull: M. F. Isacson
      – PersonEntity:
          Name:
            NameFull: M. Ishino
      – PersonEntity:
          Name:
            NameFull: W. Islam
      – PersonEntity:
          Name:
            NameFull: C. Issever
      – PersonEntity:
          Name:
            NameFull: S. Istin
      – PersonEntity:
          Name:
            NameFull: F. Ito
      – PersonEntity:
          Name:
            NameFull: J. M. Iturbe Ponce
      – PersonEntity:
          Name:
            NameFull: R. Iuppa
      – PersonEntity:
          Name:
            NameFull: A. Ivina
      – PersonEntity:
          Name:
            NameFull: H. Iwasaki
      – PersonEntity:
          Name:
            NameFull: J. M. Izen
      – PersonEntity:
          Name:
            NameFull: V. Izzo
      – PersonEntity:
          Name:
            NameFull: P. Jacka
      – PersonEntity:
          Name:
            NameFull: P. Jackson
      – PersonEntity:
          Name:
            NameFull: R. M. Jacobs
      – PersonEntity:
          Name:
            NameFull: B. P. Jaeger
      – PersonEntity:
          Name:
            NameFull: V. Jain
      – PersonEntity:
          Name:
            NameFull: G. Jäkel
      – PersonEntity:
          Name:
            NameFull: K. B. Jakobi
      – PersonEntity:
          Name:
            NameFull: K. Jakobs
      – PersonEntity:
          Name:
            NameFull: T. Jakoubek
      – PersonEntity:
          Name:
            NameFull: J. Jamieson
      – PersonEntity:
          Name:
            NameFull: K. W. Janas
      – PersonEntity:
          Name:
            NameFull: R. Jansky
      – PersonEntity:
          Name:
            NameFull: J. Janssen
      – PersonEntity:
          Name:
            NameFull: M. Janus
      – PersonEntity:
          Name:
            NameFull: P. A. Janus
      – PersonEntity:
          Name:
            NameFull: G. Jarlskog
      – PersonEntity:
          Name:
            NameFull: N. Javadov
      – PersonEntity:
          Name:
            NameFull: T. Javůrek
      – PersonEntity:
          Name:
            NameFull: M. Javurkova
      – PersonEntity:
          Name:
            NameFull: F. Jeanneau
      – PersonEntity:
          Name:
            NameFull: L. Jeanty
      – PersonEntity:
          Name:
            NameFull: J. Jejelava
      – PersonEntity:
          Name:
            NameFull: A. Jelinskas
      – PersonEntity:
          Name:
            NameFull: P. Jenni
      – PersonEntity:
          Name:
            NameFull: J. Jeong
      – PersonEntity:
          Name:
            NameFull: N. Jeong
      – PersonEntity:
          Name:
            NameFull: S. Jézéquel
      – PersonEntity:
          Name:
            NameFull: H. Ji
      – PersonEntity:
          Name:
            NameFull: J. Jia
      – PersonEntity:
          Name:
            NameFull: H. Jiang
      – PersonEntity:
          Name:
            NameFull: Y. Jiang
      – PersonEntity:
          Name:
            NameFull: Z. Jiang
      – PersonEntity:
          Name:
            NameFull: S. Jiggins
      – PersonEntity:
          Name:
            NameFull: F. A. Jimenez Morales
      – PersonEntity:
          Name:
            NameFull: J. Jimenez Pena
      – PersonEntity:
          Name:
            NameFull: S. Jin
      – PersonEntity:
          Name:
            NameFull: A. Jinaru
      – PersonEntity:
          Name:
            NameFull: O. Jinnouchi
      – PersonEntity:
          Name:
            NameFull: H. Jivan
      – PersonEntity:
          Name:
            NameFull: P. Johansson
      – PersonEntity:
          Name:
            NameFull: K. A. Johns
      – PersonEntity:
          Name:
            NameFull: C. A. Johnson
      – PersonEntity:
          Name:
            NameFull: K. Jon-And
      – PersonEntity:
          Name:
            NameFull: R. W. L. Jones
      – PersonEntity:
          Name:
            NameFull: S. D. Jones
      – PersonEntity:
          Name:
            NameFull: S. Jones
      – PersonEntity:
          Name:
            NameFull: T. J. Jones
      – PersonEntity:
          Name:
            NameFull: J. Jongmanns
      – PersonEntity:
          Name:
            NameFull: P. M. Jorge
      – PersonEntity:
          Name:
            NameFull: J. Jovicevic
      – PersonEntity:
          Name:
            NameFull: X. Ju
      – PersonEntity:
          Name:
            NameFull: J. J. Junggeburth
      – PersonEntity:
          Name:
            NameFull: A. Juste Rozas
      – PersonEntity:
          Name:
            NameFull: A. Kaczmarska
      – PersonEntity:
          Name:
            NameFull: M. Kado
      – PersonEntity:
          Name:
            NameFull: H. Kagan
      – PersonEntity:
          Name:
            NameFull: M. Kagan
      – PersonEntity:
          Name:
            NameFull: A. Kahn
      – PersonEntity:
          Name:
            NameFull: C. Kahra
      – PersonEntity:
          Name:
            NameFull: T. Kaji
      – PersonEntity:
          Name:
            NameFull: E. Kajomovitz
      – PersonEntity:
          Name:
            NameFull: C. W. Kalderon
      – PersonEntity:
          Name:
            NameFull: A. Kaluza
      – PersonEntity:
          Name:
            NameFull: A. Kamenshchikov
      – PersonEntity:
          Name:
            NameFull: M. Kaneda
      – PersonEntity:
          Name:
            NameFull: N. J. Kang
      – PersonEntity:
          Name:
            NameFull: L. Kanjir
      – PersonEntity:
          Name:
            NameFull: Y. Kano
      – PersonEntity:
          Name:
            NameFull: V. A. Kantserov
      – PersonEntity:
          Name:
            NameFull: J. Kanzaki
      – PersonEntity:
          Name:
            NameFull: L. S. Kaplan
      – PersonEntity:
          Name:
            NameFull: D. Kar
      – PersonEntity:
          Name:
            NameFull: K. Karava
      – PersonEntity:
          Name:
            NameFull: M. J. Kareem
      – PersonEntity:
          Name:
            NameFull: S. N. Karpov
      – PersonEntity:
          Name:
            NameFull: Z. M. Karpova
      – PersonEntity:
          Name:
            NameFull: V. Kartvelishvili
      – PersonEntity:
          Name:
            NameFull: A. N. Karyukhin
      – PersonEntity:
          Name:
            NameFull: L. Kashif
      – PersonEntity:
          Name:
            NameFull: R. D. Kass
      – PersonEntity:
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            NameFull: A. Kastanas
      – PersonEntity:
          Name:
            NameFull: C. Kato
      – PersonEntity:
          Name:
            NameFull: J. Katzy
      – PersonEntity:
          Name:
            NameFull: K. Kawade
      – PersonEntity:
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            NameFull: K. Kawagoe
      – PersonEntity:
          Name:
            NameFull: T. Kawaguchi
      – PersonEntity:
          Name:
            NameFull: T. Kawamoto
      – PersonEntity:
          Name:
            NameFull: G. Kawamura
      – PersonEntity:
          Name:
            NameFull: E. F. Kay
      – PersonEntity:
          Name:
            NameFull: V. F. Kazanin
      – PersonEntity:
          Name:
            NameFull: R. Keeler
      – PersonEntity:
          Name:
            NameFull: R. Kehoe
      – PersonEntity:
          Name:
            NameFull: J. S. Keller
      – PersonEntity:
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            NameFull: E. Kellermann
      – PersonEntity:
          Name:
            NameFull: D. Kelsey
      – PersonEntity:
          Name:
            NameFull: J. J. Kempster
      – PersonEntity:
          Name:
            NameFull: J. Kendrick
      – PersonEntity:
          Name:
            NameFull: K. E. Kennedy
      – PersonEntity:
          Name:
            NameFull: O. Kepka
      – PersonEntity:
          Name:
            NameFull: S. Kersten
      – PersonEntity:
          Name:
            NameFull: B. P. Kerševan
      – PersonEntity:
          Name:
            NameFull: S. Ketabchi Haghighat
      – PersonEntity:
          Name:
            NameFull: M. Khader
      – PersonEntity:
          Name:
            NameFull: F. Khalil-Zada
      – PersonEntity:
          Name:
            NameFull: M. Khandoga
      – PersonEntity:
          Name:
            NameFull: A. Khanov
      – PersonEntity:
          Name:
            NameFull: A. G. Kharlamov
      – PersonEntity:
          Name:
            NameFull: T. Kharlamova
      – PersonEntity:
          Name:
            NameFull: E. E. Khoda
      – PersonEntity:
          Name:
            NameFull: A. Khodinov
      – PersonEntity:
          Name:
            NameFull: T. J. Khoo
      – PersonEntity:
          Name:
            NameFull: E. Khramov
      – PersonEntity:
          Name:
            NameFull: J. Khubua
      – PersonEntity:
          Name:
            NameFull: S. Kido
      – PersonEntity:
          Name:
            NameFull: M. Kiehn
      – PersonEntity:
          Name:
            NameFull: C. R. Kilby
      – PersonEntity:
          Name:
            NameFull: Y. K. Kim
      – PersonEntity:
          Name:
            NameFull: N. Kimura
      – PersonEntity:
          Name:
            NameFull: O. M. Kind
      – PersonEntity:
          Name:
            NameFull: B. T. King
      – PersonEntity:
          Name:
            NameFull: D. Kirchmeier
      – PersonEntity:
          Name:
            NameFull: J. Kirk
      – PersonEntity:
          Name:
            NameFull: A. E. Kiryunin
      – PersonEntity:
          Name:
            NameFull: T. Kishimoto
      – PersonEntity:
          Name:
            NameFull: D. P. Kisliuk
      – PersonEntity:
          Name:
            NameFull: V. Kitali
      – PersonEntity:
          Name:
            NameFull: O. Kivernyk
      – PersonEntity:
          Name:
            NameFull: T. Klapdor-Kleingrothaus
      – PersonEntity:
          Name:
            NameFull: M. Klassen
      – PersonEntity:
          Name:
            NameFull: M. H. Klein
      – PersonEntity:
          Name:
            NameFull: M. Klein
      – PersonEntity:
          Name:
            NameFull: U. Klein
      – PersonEntity:
          Name:
            NameFull: K. Kleinknecht
      – PersonEntity:
          Name:
            NameFull: P. Klimek
      – PersonEntity:
          Name:
            NameFull: A. Klimentov
      – PersonEntity:
          Name:
            NameFull: T. Klingl
      – PersonEntity:
          Name:
            NameFull: T. Klioutchnikova
      – PersonEntity:
          Name:
            NameFull: F. F. Klitzner
      – PersonEntity:
          Name:
            NameFull: P. Kluit
      – PersonEntity:
          Name:
            NameFull: S. Kluth
      – PersonEntity:
          Name:
            NameFull: E. Kneringer
      – PersonEntity:
          Name:
            NameFull: E. B. F. G. Knoops
      – PersonEntity:
          Name:
            NameFull: A. Knue
      – PersonEntity:
          Name:
            NameFull: D. Kobayashi
      – PersonEntity:
          Name:
            NameFull: T. Kobayashi
      – PersonEntity:
          Name:
            NameFull: M. Kobel
      – PersonEntity:
          Name:
            NameFull: M. Kocian
      – PersonEntity:
          Name:
            NameFull: P. Kodys
      – PersonEntity:
          Name:
            NameFull: P. T. Koenig
      – PersonEntity:
          Name:
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            NameFull: J. Levêque
      – PersonEntity:
          Name:
            NameFull: D. Levin
      – PersonEntity:
          Name:
            NameFull: L. J. Levinson
      – PersonEntity:
          Name:
            NameFull: D. J. Lewis
      – PersonEntity:
          Name:
            NameFull: B. Li
      – PersonEntity:
          Name:
            NameFull: C-Q. Li
      – PersonEntity:
          Name:
            NameFull: F. Li
      – PersonEntity:
          Name:
            NameFull: H. Li
      – PersonEntity:
          Name:
            NameFull: J. Li
      – PersonEntity:
          Name:
            NameFull: K. Li
      – PersonEntity:
          Name:
            NameFull: L. Li
      – PersonEntity:
          Name:
            NameFull: M. Li
      – PersonEntity:
          Name:
            NameFull: Q. Li
      – PersonEntity:
          Name:
            NameFull: Q. Y. Li
      – PersonEntity:
          Name:
            NameFull: S. Li
      – PersonEntity:
          Name:
            NameFull: X. Li
      – PersonEntity:
          Name:
            NameFull: Y. Li
      – PersonEntity:
          Name:
            NameFull: Z. Li
      – PersonEntity:
          Name:
            NameFull: Z. Liang
      – PersonEntity:
          Name:
            NameFull: B. Liberti
      – PersonEntity:
          Name:
            NameFull: A. Liblong
      – PersonEntity:
          Name:
            NameFull: K. Lie
      – PersonEntity:
          Name:
            NameFull: S. Lim
      – PersonEntity:
          Name:
            NameFull: C. Y. Lin
      – PersonEntity:
          Name:
            NameFull: K. Lin
      – PersonEntity:
          Name:
            NameFull: T. H. Lin
      – PersonEntity:
          Name:
            NameFull: R. A. Linck
      – PersonEntity:
          Name:
            NameFull: J. H. Lindon
      – PersonEntity:
          Name:
            NameFull: A. L. Lionti
      – PersonEntity:
          Name:
            NameFull: E. Lipeles
      – PersonEntity:
          Name:
            NameFull: A. Lipniacka
      – PersonEntity:
          Name:
            NameFull: T. M. Liss
      – PersonEntity:
          Name:
            NameFull: A. Lister
      – PersonEntity:
          Name:
            NameFull: A. M. Litke
      – PersonEntity:
          Name:
            NameFull: J. D. Little
      – PersonEntity:
          Name:
            NameFull: B. Liu
      – PersonEntity:
          Name:
            NameFull: B. L. Liu
      – PersonEntity:
          Name:
            NameFull: H. B. Liu
      – PersonEntity:
          Name:
            NameFull: H. Liu
      – PersonEntity:
          Name:
            NameFull: J. B. Liu
      – PersonEntity:
          Name:
            NameFull: J. K. K. Liu
      – PersonEntity:
          Name:
            NameFull: K. Liu
      – PersonEntity:
          Name:
            NameFull: M. Liu
      – PersonEntity:
          Name:
            NameFull: P. Liu
      – PersonEntity:
          Name:
            NameFull: Y. Liu
      – PersonEntity:
          Name:
            NameFull: Y. L. Liu
      – PersonEntity:
          Name:
            NameFull: Y. W. Liu
      – PersonEntity:
          Name:
            NameFull: M. Livan
      – PersonEntity:
          Name:
            NameFull: A. Lleres
      – PersonEntity:
          Name:
            NameFull: J. Llorente Merino
      – PersonEntity:
          Name:
            NameFull: S. L. Lloyd
      – PersonEntity:
          Name:
            NameFull: C. Y. Lo
      – PersonEntity:
          Name:
            NameFull: F. Lo Sterzo
      – PersonEntity:
          Name:
            NameFull: E. M. Lobodzinska
      – PersonEntity:
          Name:
            NameFull: P. Loch
      – PersonEntity:
          Name:
            NameFull: S. Loffredo
      – PersonEntity:
          Name:
            NameFull: T. Lohse
      – PersonEntity:
          Name:
            NameFull: K. Lohwasser
      – PersonEntity:
          Name:
            NameFull: M. Lokajicek
      – PersonEntity:
          Name:
            NameFull: J. D. Long
      – PersonEntity:
          Name:
            NameFull: R. E. Long
      – PersonEntity:
          Name:
            NameFull: L. Longo
      – PersonEntity:
          Name:
            NameFull: K. A. Looper
      – PersonEntity:
          Name:
            NameFull: J. A. Lopez
      – PersonEntity:
          Name:
            NameFull: I. Lopez Paz
      – PersonEntity:
          Name:
            NameFull: A. Lopez Solis
      – PersonEntity:
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            NameFull: J. Lorenz
      – PersonEntity:
          Name:
            NameFull: N. Lorenzo Martinez
      – PersonEntity:
          Name:
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      – PersonEntity:
          Name:
            NameFull: M. Losada
      – PersonEntity:
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      – PersonEntity:
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            NameFull: A. Lösle
      – PersonEntity:
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            NameFull: X. Lou
      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
          Name:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
          Name:
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      – PersonEntity:
          Name:
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      – PersonEntity:
          Name:
            NameFull: C. Luci
      – PersonEntity:
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      – PersonEntity:
          Name:
            NameFull: C. Luedtke
      – PersonEntity:
          Name:
            NameFull: F. Luehring
      – PersonEntity:
          Name:
            NameFull: I. Luise
      – PersonEntity:
          Name:
            NameFull: L. Luminari
      – PersonEntity:
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            NameFull: B. Lund-Jensen
      – PersonEntity:
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      – PersonEntity:
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            NameFull: D. Lynn
      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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            NameFull: T. Lyubushkina
      – PersonEntity:
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            NameFull: H. Ma
      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
          Name:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
          Name:
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      – PersonEntity:
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      – PersonEntity:
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            NameFull: N. Madysa
      – PersonEntity:
          Name:
            NameFull: J. Maeda
      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
          Name:
            NameFull: N. Magini
      – PersonEntity:
          Name:
            NameFull: D. J. Mahon
      – PersonEntity:
          Name:
            NameFull: C. Maidantchik
      – PersonEntity:
          Name:
            NameFull: T. Maier
      – PersonEntity:
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            NameFull: A. Maio
      – PersonEntity:
          Name:
            NameFull: K. Maj
      – PersonEntity:
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      – PersonEntity:
          Name:
            NameFull: S. Majewski
      – PersonEntity:
          Name:
            NameFull: Y. Makida
      – PersonEntity:
          Name:
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      – PersonEntity:
          Name:
            NameFull: B. Malaescu
      – PersonEntity:
          Name:
            NameFull: Pa. Malecki
      – PersonEntity:
          Name:
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      – PersonEntity:
          Name:
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      – PersonEntity:
          Name:
            NameFull: U. Mallik
      – PersonEntity:
          Name:
            NameFull: D. Malon
      – PersonEntity:
          Name:
            NameFull: C. Malone
      – PersonEntity:
          Name:
            NameFull: S. Maltezos
      – PersonEntity:
          Name:
            NameFull: S. Malyukov
      – PersonEntity:
          Name:
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      – PersonEntity:
          Name:
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      – PersonEntity:
          Name:
            NameFull: I. Mandić
      – PersonEntity:
          Name:
            NameFull: L. Manhaes de Andrade Filho
      – PersonEntity:
          Name:
            NameFull: I. M. Maniatis
      – PersonEntity:
          Name:
            NameFull: J. Manjarres Ramos
      – PersonEntity:
          Name:
            NameFull: K. H. Mankinen
      – PersonEntity:
          Name:
            NameFull: A. Mann
      – PersonEntity:
          Name:
            NameFull: A. Manousos
      – PersonEntity:
          Name:
            NameFull: B. Mansoulie
      – PersonEntity:
          Name:
            NameFull: I. Manthos
      – PersonEntity:
          Name:
            NameFull: S. Manzoni
      – PersonEntity:
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            NameFull: A. Marantis
      – PersonEntity:
          Name:
            NameFull: G. Marceca
      – PersonEntity:
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            NameFull: L. Marchese
      – PersonEntity:
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            NameFull: G. Marchiori
      – PersonEntity:
          Name:
            NameFull: M. Marcisovsky
      – PersonEntity:
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            NameFull: L. Marcoccia
      – PersonEntity:
          Name:
            NameFull: C. Marcon
      – PersonEntity:
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      – PersonEntity:
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            NameFull: M. Marjanovic
      – PersonEntity:
          Name:
            NameFull: Z. Marshall
      – PersonEntity:
          Name:
            NameFull: M. U. F. Martensson
      – PersonEntity:
          Name:
            NameFull: S. Marti-Garcia
      – PersonEntity:
          Name:
            NameFull: C. B. Martin
      – PersonEntity:
          Name:
            NameFull: T. A. Martin
      – PersonEntity:
          Name:
            NameFull: V. J. Martin
      – PersonEntity:
          Name:
            NameFull: B. Martin dit Latour
      – PersonEntity:
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            NameFull: L. Martinelli
      – PersonEntity:
          Name:
            NameFull: M. Martinez
      – PersonEntity:
          Name:
            NameFull: V. I. Martinez Outschoorn
      – PersonEntity:
          Name:
            NameFull: S. Martin-Haugh
      – PersonEntity:
          Name:
            NameFull: V. S. Martoiu
      – PersonEntity:
          Name:
            NameFull: A. C. Martyniuk
      – PersonEntity:
          Name:
            NameFull: A. Marzin
      – PersonEntity:
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            NameFull: S. R. Maschek
      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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            NameFull: R. Röhrig
      – PersonEntity:
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            NameFull: R. A. Rojas
      – PersonEntity:
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            NameFull: C. P. A. Roland
      – PersonEntity:
          Name:
            NameFull: J. Roloff
      – PersonEntity:
          Name:
            NameFull: A. Romaniouk
      – PersonEntity:
          Name:
            NameFull: M. Romano
      – PersonEntity:
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            NameFull: N. Rompotis
      – PersonEntity:
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            NameFull: M. Ronzani
      – PersonEntity:
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            NameFull: L. Roos
      – PersonEntity:
          Name:
            NameFull: S. Rosati
      – PersonEntity:
          Name:
            NameFull: G. Rosin
      – PersonEntity:
          Name:
            NameFull: B. J. Rosser
      – PersonEntity:
          Name:
            NameFull: E. Rossi
      – PersonEntity:
          Name:
            NameFull: L. P. Rossi
      – PersonEntity:
          Name:
            NameFull: L. Rossini
      – PersonEntity:
          Name:
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      – PersonEntity:
          Name:
            NameFull: M. Rotaru
      – PersonEntity:
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            NameFull: J. Rothberg
      – PersonEntity:
          Name:
            NameFull: D. Rousseau
      – PersonEntity:
          Name:
            NameFull: G. Rovelli
      – PersonEntity:
          Name:
            NameFull: A. Roy
      – PersonEntity:
          Name:
            NameFull: D. Roy
      – PersonEntity:
          Name:
            NameFull: A. Rozanov
      – PersonEntity:
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            NameFull: Y. Rozen
      – PersonEntity:
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            NameFull: X. Ruan
      – PersonEntity:
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      – PersonEntity:
          Name:
            NameFull: A. Ruiz-Martinez
      – PersonEntity:
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            NameFull: A. Rummler
      – PersonEntity:
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            NameFull: Z. Rurikova
      – PersonEntity:
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            NameFull: N. A. Rusakovich
      – PersonEntity:
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      – PersonEntity:
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            NameFull: L. Rustige
      – PersonEntity:
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            NameFull: J. P. Rutherfoord
      – PersonEntity:
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            NameFull: E. M. Rüttinger
      – PersonEntity:
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            NameFull: M. Rybar
      – PersonEntity:
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            NameFull: G. Rybkin
      – PersonEntity:
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            NameFull: E. B. Rye
      – PersonEntity:
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            NameFull: A. Ryzhov
      – PersonEntity:
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            NameFull: J. A. Sabater Iglesias
      – PersonEntity:
          Name:
            NameFull: P. Sabatini
      – PersonEntity:
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            NameFull: G. Sabato
      – PersonEntity:
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            NameFull: S. Sacerdoti
      – PersonEntity:
          Name:
            NameFull: H.F-W. Sadrozinski
      – PersonEntity:
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            NameFull: R. Sadykov
      – PersonEntity:
          Name:
            NameFull: F. Safai Tehrani
      – PersonEntity:
          Name:
            NameFull: B. Safarzadeh Samani
      – PersonEntity:
          Name:
            NameFull: P. Saha
      – PersonEntity:
          Name:
            NameFull: S. Saha
      – PersonEntity:
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            NameFull: M. Sahinsoy
      – PersonEntity:
          Name:
            NameFull: A. Sahu
      – PersonEntity:
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            NameFull: M. Saimpert
      – PersonEntity:
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            NameFull: M. Saito
      – PersonEntity:
          Name:
            NameFull: T. Saito
      – PersonEntity:
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            NameFull: H. Sakamoto
      – PersonEntity:
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      – PersonEntity:
          Name:
            NameFull: D. Salamani
      – PersonEntity:
          Name:
            NameFull: G. Salamanna
      – PersonEntity:
          Name:
            NameFull: J. E. Salazar Loyola
      – PersonEntity:
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            NameFull: A. Salnikov
      – PersonEntity:
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            NameFull: J. Salt
      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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            NameFull: A. Salvucci
      – PersonEntity:
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            NameFull: A. Salzburger
      – PersonEntity:
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      – PersonEntity:
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            NameFull: D. Sammel
      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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            NameFull: Y. Sano
      – PersonEntity:
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            NameFull: A. Sansoni
      – PersonEntity:
          Name:
            NameFull: C. Santoni
      – PersonEntity:
          Name:
            NameFull: H. Santos
      – PersonEntity:
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      – PersonEntity:
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            NameFull: A. Santra
      – PersonEntity:
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      – PersonEntity:
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            NameFull: J. G. Saraiva
      – PersonEntity:
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            NameFull: O. Sasaki
      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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            NameFull: R. Sawada
      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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            NameFull: L. Schaefer
      – PersonEntity:
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      – PersonEntity:
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            NameFull: S. Schaepe
      – PersonEntity:
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            NameFull: U. Schäfer
      – PersonEntity:
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      – PersonEntity:
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            NameFull: D. Schaile
      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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            NameFull: D. Scheirich
      – PersonEntity:
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            NameFull: F. Schenck
      – PersonEntity:
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            NameFull: M. Schernau
      – PersonEntity:
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            NameFull: C. Schiavi
      – PersonEntity:
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            NameFull: S. Schier
      – PersonEntity:
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      – PersonEntity:
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            NameFull: Z. M. Schillaci
      – PersonEntity:
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            NameFull: E. J. Schioppa
      – PersonEntity:
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            NameFull: M. Schioppa
      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
          Name:
            NameFull: K. R. Schmidt-Sommerfeld
      – PersonEntity:
          Name:
            NameFull: K. Schmieden
      – PersonEntity:
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            NameFull: C. Schmitt
      – PersonEntity:
          Name:
            NameFull: S. Schmitt
      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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            NameFull: U. Schnoor
      – PersonEntity:
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            NameFull: L. Schoeffel
      – PersonEntity:
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            NameFull: A. Schoening
      – PersonEntity:
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      – PersonEntity:
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            NameFull: E. Schopf
      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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            NameFull: S. Schramm
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            NameFull: F. Schroeder
      – PersonEntity:
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            NameFull: A. Schulte
      – PersonEntity:
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      – PersonEntity:
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            NameFull: M. Schumacher
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      – PersonEntity:
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            NameFull: Ph. Schune
      – PersonEntity:
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            NameFull: A. Schwartzman
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      – PersonEntity:
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      – PersonEntity:
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            NameFull: R. Schwienhorst
      – PersonEntity:
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      – PersonEntity:
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            NameFull: M. Scodeggio
      – PersonEntity:
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            NameFull: M. Scornajenghi
      – PersonEntity:
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            NameFull: F. Scuri
      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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            NameFull: P. Seema
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      – PersonEntity:
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            NameFull: A. Seiden
      – PersonEntity:
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      – PersonEntity:
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            NameFull: T. Seiss
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            NameFull: G. Sekhniaidze
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            NameFull: K. Sekhon
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            NameFull: S. J. Sekula
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            NameFull: N. Semprini-Cesari
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            NameFull: S. Sen
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      – PersonEntity:
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      – PersonEntity:
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            NameFull: M. Vanadia
      – PersonEntity:
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            NameFull: W. Vandelli
      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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            NameFull: A. Vaniachine
      – PersonEntity:
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            NameFull: D. Vannicola
      – PersonEntity:
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            NameFull: R. Vari
      – PersonEntity:
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      – PersonEntity:
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            NameFull: C. Varni
      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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            NameFull: J. Veatch
      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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            NameFull: E. Vilucchi
      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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            NameFull: J. Wang
      – PersonEntity:
          Name:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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            NameFull: R. Wang
      – PersonEntity:
          Name:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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            NameFull: E. Winkels
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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      – PersonEntity:
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    IsPartOfRelationships:
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          Dates:
            – D: 01
              M: 06
              Type: published
              Y: 2020
          Identifiers:
            – Type: issn-print
              Value: 14346044
            – Type: issn-print
              Value: 14346052
          Numbering:
            – Type: volume
              Value: 80
            – Type: issue
              Value: 6
          Titles:
            – TitleFull: European Physical Journal C: Particles and Fields
              Type: main
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