Herschel 158 μm [C II] Observations of "CO-dark" Gas in the Perseus Giant Molecular Cloud

被引:3
|
作者
Hall, K. P. [1 ]
Stanimirovic, Snezana [1 ]
Lee, Min-Young [2 ,3 ]
Wolfire, Mark [4 ]
Goldsmith, Paul [5 ]
机构
[1] Univ Wisconsin, Dept Astron, 475 North Charter St, Madison, WI 53706 USA
[2] Korea Astron & Space Sci Inst, 776 Daedeokdae Ro, Daejeon 34055, South Korea
[3] Max Planck Inst Radio Astron, Hugel 69, D-53121 Bonn, Germany
[4] Univ Maryland, Dept Astron, College Pk, MD 20742 USA
[5] CALTECH, Jet Prop Lab, 4800 Oak Grove Dr, Pasadena, CA 91109 USA
来源
ASTROPHYSICAL JOURNAL | 2020年 / 899卷 / 01期
基金
美国国家科学基金会;
关键词
Giant molecular clouds; Interstellar clouds; Molecular gas; Diffuse molecular clouds; Dark interstellar clouds; Photodissociation regions; Astronomy data modeling; Astronomy data analysis; Far infrared astronomy; PHOTODISSOCIATION REGIONS; INTERSTELLAR-MEDIUM; X-FACTOR; INFRARED OBSERVATIONS; DENSITY; EMISSION; SPACE; PDR; !text type='PYTHON']PYTHON[!/text; ARRAY;
D O I
10.3847/1538-4357/ab9b86
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We present observations of velocity-resolved [C II] 158 mu m emission from both a dense and a more diffuse photodissociation region (PDR) in the Perseus giant molecular cloud using the Heterodyne Instrument for the Far-Infrared on board the Herschel Space Telescope. We detect [C II] emission from 80% of the total positions, with a 95% detection rate from the dense boundary region. The integrated intensity of the [C II] emission remains relatively constant across each boundary, despite the observed range in optical extinction between 1 and 10 mag. This flat profile indicates a constant heating and cooling rate within both regions observed. The integrated intensity of [C II] emission is reasonably well correlated with the neutral hydrogen (H I) column density, as well as the total gas column density. This, in addition to the 80' (7 pc) extent of the [C II] emission from the cloud center, suggests that the H I envelope plays a dominant role in explaining the [C II] emission emanating from Perseus. We compare the [C II] and (CO)-C-12 integrated intensities with predictions from a 1D, two-sided slab PDR model and show that a simple core + envelope, equilibrium model without an additional "CO-dark" H-2 component can reproduce observations well. Additional observations are needed to disentangle how much of the [C II] emission is associated with the "CO-dark" H-2 gas, as well as constrain spatial variations of the dust-to-gas ratio across Perseus.
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页数:20
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