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Where is OH and does it trace the dark molecular gas (DMG)?
Citation
Li, D and Tang, N and Nguyen, H and Dawson, JR and Heiles, C and Xu, D and Pan, Z and Goldsmith, PF and Gibson, SJ and Murray, CE and Robishaw, T and McClure-Griffiths, NM and Dickey, J and Pineda, J and Stanimirovic, S and Bronfman, L and Troland, T and the PRIMO Collaboration, Where is OH and does it trace the dark molecular gas (DMG)?, Astrophysical Journal Supplement Series, 235, (1) Article 1. ISSN 0067-0049 (2018) [Refereed Article]
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Copyright Statement
Copyright 2018 The American Astronomical Society
DOI: doi:10.3847/1538-4365/aaa762
Abstract
Hydroxyl (OH) is expected to be abundant in diffuse interstellar molecular gas because it forms along with H2 under similar conditions and forms within a similar extinction range. We have analyzed absorption measurements of OH at 1665 MHz and 1667 MHz toward 44 extragalactic continuum sources, together with the J = 1–0 transitions of 12CO, 13CO, and C18O, and the J = 2–1 transition of 12CO. The excitation temperatures of OH were found to follow a modified lognormal distribution
the peak of which is close to the temperature of the Galactic emission background (CMB+synchrotron). In fact, 90% of the OH has excitation temperatures within 2 K of the Galactic background at the same location, providing a plausible explanation for the apparent difficulty of mapping this abundant molecule in emission. The opacities of OH were found to be small and to peak around 0.01. For gas at intermediate extinctions (AV ~ 0.05–2 mag), the detection rate of OH with a detection limit N(OH)
1012 cm−2 is approximately independent of AV. We conclude that OH is abundant in the diffuse molecular gas and OH absorption is a good tracer of "dark molecular gas (DMG)." The measured fraction of DMG depends on the assumed detection threshold of the CO data set. The next generation of highly sensitive low-frequency radio telescopes, such as FAST and SKA, will make feasible the systematic inventory of diffuse molecular gas through decomposing, in velocity, the molecular (e.g., OH and CH) absorption profiles toward background continuum sources with numbers exceeding what is currently available by orders of magnitude.
![$f({T}_{\mathrm{ex}})\propto \tfrac{1}{\sqrt{2\pi }\sigma }\exp \left[-\tfrac{{[\mathrm{ln}({T}_{\mathrm{ex}})-\mathrm{ln}(3.4{\rm{K}})]}^{2}}{2{\sigma }^{2}}\right],$](https://cdn.iopscience.com/images/0067-0049/235/1/1/apjsaaa762ieqn1.gif)

Item Details
Item Type: | Refereed Article |
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Keywords: | radio astronomy, gas clouds, evolution, molecules |
Research Division: | Physical Sciences |
Research Group: | Astronomical sciences |
Research Field: | Galactic astronomy |
Objective Division: | Expanding Knowledge |
Objective Group: | Expanding knowledge |
Objective Field: | Expanding knowledge in the physical sciences |
UTAS Author: | Dickey, J (Professor John Dickey) |
ID Code: | 133230 |
Year Published: | 2018 |
Web of Science® Times Cited: | 31 |
Deposited By: | Mathematics and Physics |
Deposited On: | 2019-06-19 |
Last Modified: | 2019-07-29 |
Downloads: | 15 View Download Statistics |
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