Origin of warm and hot gas emission from low-mass protostars: Herschel-HIFI observations of CO J=16-15. I. Line profiles, physical conditions, and H2O abundance
Title: | Origin of warm and hot gas emission from low-mass protostars: Herschel-HIFI observations of CO J=16-15. I. Line profiles, physical conditions, and H2O abundance |
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Authors: | Kristensen, L. E., van Dishoeck, E. F., Mottram, J. C., Karska, A., Yildiz, U. A., Bergin, E. A., Bjerkeli, P., Cabrit, S., Doty, S., Evans II, N. J., Gusdorf, A., Harsono, D., Herczeg, G. J., Johnstone, D., Jørgensen, J. K., van Kempen, T. A., Lee, J. -E., Maret, S., Tafalla, M., Visser, R., Wampfler, S. F. |
Source: | A&A 605, A93 (2017) |
Publication Year: | 2017 |
Collection: | Astrophysics |
Subject Terms: | Astrophysics - Astrophysics of Galaxies, Astrophysics - Solar and Stellar Astrophysics |
More Details: | (Abridged) Through spectrally unresolved observations of high-J CO transitions, Herschel-PACS has revealed large reservoirs of warm (300 K) and hot (700 K) molecular gas around low-mass protostars. We aim to shed light on the excitation and origin of the CO ladder observed toward protostars, and on the water abundance in different physical components using spectrally resolved Herschel-HIFI data. Observations are presented of the highly excited CO line J=16-15 with Herschel-HIFI toward 24 low-mass protostellar objects. The spectrally resolved profiles show two distinct velocity components: a broad component with an average FWHM of 20 km/s, and a narrower component with a FWHM of 5 km/s that is often offset from the source velocity. The average rotational temperature over the entire profile, as measured from comparison between CO J=16-15 and 10-9 emission, is ~300 K. A radiative-transfer analysis shows that the average H2O/CO column-density ratio is ~0.02, suggesting a total H2O abundance of ~2x10^-6. Two distinct velocity profiles observed in the HIFI line profiles suggest that the CO ladder observed with PACS consists of two excitation components. The warm component (300 K) is associated with the broad HIFI component, and the hot component (700 K) is associated with the offset HIFI component. The former originates in either outflow cavity shocks or the disk wind, and the latter in irradiated shocks. The ubiquity of the warm and hot CO components suggests that fundamental mechanisms govern the excitation of these components; we hypothesize that the warm component arises when H2 stops being the dominant coolant. In this scenario, the hot component arises in cooling molecular H2-poor gas just prior to the onset of H2 formation. High spectral resolution observations of highly excited CO transitions uniquely shed light on the origin of warm and hot gas in low-mass protostellar objects. Comment: Accepted for publication in A&A |
Document Type: | Working Paper |
DOI: | 10.1051/0004-6361/201630127 |
Access URL: | http://arxiv.org/abs/1705.10269 |
Accession Number: | edsarx.1705.10269 |
Database: | arXiv |
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A.</searchLink><br /><searchLink fieldCode="AR" term="%22Bjerkeli%2C+P%2E%22">Bjerkeli, P.</searchLink><br /><searchLink fieldCode="AR" term="%22Cabrit%2C+S%2E%22">Cabrit, S.</searchLink><br /><searchLink fieldCode="AR" term="%22Doty%2C+S%2E%22">Doty, S.</searchLink><br /><searchLink fieldCode="AR" term="%22Evans+II%2C+N%2E+J%2E%22">Evans II, N. J.</searchLink><br /><searchLink fieldCode="AR" term="%22Gusdorf%2C+A%2E%22">Gusdorf, A.</searchLink><br /><searchLink fieldCode="AR" term="%22Harsono%2C+D%2E%22">Harsono, D.</searchLink><br /><searchLink fieldCode="AR" term="%22Herczeg%2C+G%2E+J%2E%22">Herczeg, G. J.</searchLink><br /><searchLink fieldCode="AR" term="%22Johnstone%2C+D%2E%22">Johnstone, D.</searchLink><br /><searchLink fieldCode="AR" term="%22Jørgensen%2C+J%2E+K%2E%22">Jørgensen, J. K.</searchLink><br /><searchLink fieldCode="AR" term="%22van+Kempen%2C+T%2E+A%2E%22">van Kempen, T. A.</searchLink><br /><searchLink fieldCode="AR" term="%22Lee%2C+J%2E+-E%2E%22">Lee, J. -E.</searchLink><br /><searchLink fieldCode="AR" term="%22Maret%2C+S%2E%22">Maret, S.</searchLink><br /><searchLink fieldCode="AR" term="%22Tafalla%2C+M%2E%22">Tafalla, M.</searchLink><br /><searchLink fieldCode="AR" term="%22Visser%2C+R%2E%22">Visser, R.</searchLink><br /><searchLink fieldCode="AR" term="%22Wampfler%2C+S%2E+F%2E%22">Wampfler, S. F.</searchLink> – Name: TitleSource Label: Source Group: Src Data: A&A 605, A93 (2017) – Name: DatePubCY Label: Publication Year Group: Date Data: 2017 – Name: Subset Label: Collection Group: HoldingsInfo Data: Astrophysics – Name: Subject Label: Subject Terms Group: Su Data: <searchLink fieldCode="DE" term="%22Astrophysics+-+Astrophysics+of+Galaxies%22">Astrophysics - Astrophysics of Galaxies</searchLink><br /><searchLink fieldCode="DE" term="%22Astrophysics+-+Solar+and+Stellar+Astrophysics%22">Astrophysics - Solar and Stellar Astrophysics</searchLink> – Name: Abstract Label: Description Group: Ab Data: (Abridged) Through spectrally unresolved observations of high-J CO transitions, Herschel-PACS has revealed large reservoirs of warm (300 K) and hot (700 K) molecular gas around low-mass protostars. We aim to shed light on the excitation and origin of the CO ladder observed toward protostars, and on the water abundance in different physical components using spectrally resolved Herschel-HIFI data. Observations are presented of the highly excited CO line J=16-15 with Herschel-HIFI toward 24 low-mass protostellar objects. The spectrally resolved profiles show two distinct velocity components: a broad component with an average FWHM of 20 km/s, and a narrower component with a FWHM of 5 km/s that is often offset from the source velocity. The average rotational temperature over the entire profile, as measured from comparison between CO J=16-15 and 10-9 emission, is ~300 K. A radiative-transfer analysis shows that the average H2O/CO column-density ratio is ~0.02, suggesting a total H2O abundance of ~2x10^-6. Two distinct velocity profiles observed in the HIFI line profiles suggest that the CO ladder observed with PACS consists of two excitation components. The warm component (300 K) is associated with the broad HIFI component, and the hot component (700 K) is associated with the offset HIFI component. The former originates in either outflow cavity shocks or the disk wind, and the latter in irradiated shocks. The ubiquity of the warm and hot CO components suggests that fundamental mechanisms govern the excitation of these components; we hypothesize that the warm component arises when H2 stops being the dominant coolant. In this scenario, the hot component arises in cooling molecular H2-poor gas just prior to the onset of H2 formation. High spectral resolution observations of highly excited CO transitions uniquely shed light on the origin of warm and hot gas in low-mass protostellar objects.<br />Comment: Accepted for publication in A&A – Name: TypeDocument Label: Document Type Group: TypDoc Data: Working Paper – Name: DOI Label: DOI Group: ID Data: 10.1051/0004-6361/201630127 – Name: URL Label: Access URL Group: URL Data: <link linkTarget="URL" linkTerm="http://arxiv.org/abs/1705.10269" linkWindow="_blank">http://arxiv.org/abs/1705.10269</link> – Name: AN Label: Accession Number Group: ID Data: edsarx.1705.10269 |
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RecordInfo | BibRecord: BibEntity: Identifiers: – Type: doi Value: 10.1051/0004-6361/201630127 Subjects: – SubjectFull: Astrophysics - Astrophysics of Galaxies Type: general – SubjectFull: Astrophysics - Solar and Stellar Astrophysics Type: general Titles: – TitleFull: Origin of warm and hot gas emission from low-mass protostars: Herschel-HIFI observations of CO J=16-15. I. Line profiles, physical conditions, and H2O abundance Type: main BibRelationships: HasContributorRelationships: – PersonEntity: Name: NameFull: Kristensen, L. E. – PersonEntity: Name: NameFull: van Dishoeck, E. F. – PersonEntity: Name: NameFull: Mottram, J. C. – PersonEntity: Name: NameFull: Karska, A. – PersonEntity: Name: NameFull: Yildiz, U. A. – PersonEntity: Name: NameFull: Bergin, E. A. – PersonEntity: Name: NameFull: Bjerkeli, P. – PersonEntity: Name: NameFull: Cabrit, S. – PersonEntity: Name: NameFull: Doty, S. – PersonEntity: Name: NameFull: Evans II, N. J. – PersonEntity: Name: NameFull: Gusdorf, A. – PersonEntity: Name: NameFull: Harsono, D. – PersonEntity: Name: NameFull: Herczeg, G. J. – PersonEntity: Name: NameFull: Johnstone, D. – PersonEntity: Name: NameFull: Jørgensen, J. K. – PersonEntity: Name: NameFull: van Kempen, T. A. – PersonEntity: Name: NameFull: Lee, J. -E. – PersonEntity: Name: NameFull: Maret, S. – PersonEntity: Name: NameFull: Tafalla, M. – PersonEntity: Name: NameFull: Visser, R. – PersonEntity: Name: NameFull: Wampfler, S. F. IsPartOfRelationships: – BibEntity: Dates: – D: 29 M: 05 Type: published Y: 2017 |
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