2019
DOI: 10.3847/1538-4357/ab3a4b
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The Structure of Dark Molecular Gas in the Galaxy. II. Physical State of “CO-dark” Gas in the Perseus Arm

Abstract: We report the results from a new, highly sensitive (∆T mb ∼ 3mK) survey for thermal OH emission at 1665 and 1667 MHz over a dense, 9 x 9-pixel grid covering a 1 • × 1 • patch of sky in the direction of l = 105. • 00, b = +2. • 50 towards the Perseus spiral arm of our Galaxy. We compare our Green Bank Telescope (GBT) 1667 MHz OH results with archival 12 CO(1-0) observations from the Five College Radio Astronomy Observatory (FCRAO) Outer Galaxy Survey within the velocity range of the Perseus Arm at these galacti… Show more

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Cited by 19 publications
(25 citation statements)
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“…While these average volume densities are not high enough to be observationally probed by CO-bright molecular gas manifesting at n 200 cm −3 (see e.g. Busch et al 2019), they are consistent with densities of so-called "CO-dark" gas, a phase associated with warmer, more diffuse molecular hydrogen which is not detectable in CO or HI. While invisible in both CO and HI, γ ray observations -capable of tracing a cloud's gas mass independent of its chemical state -show that diffuse molecular gas surrounds all nearby CO-detected molecular clouds targeted in this study.…”
Section: Chemical Transition Between Atomic and Molecular Gasmentioning
confidence: 62%
“…While these average volume densities are not high enough to be observationally probed by CO-bright molecular gas manifesting at n 200 cm −3 (see e.g. Busch et al 2019), they are consistent with densities of so-called "CO-dark" gas, a phase associated with warmer, more diffuse molecular hydrogen which is not detectable in CO or HI. While invisible in both CO and HI, γ ray observations -capable of tracing a cloud's gas mass independent of its chemical state -show that diffuse molecular gas surrounds all nearby CO-detected molecular clouds targeted in this study.…”
Section: Chemical Transition Between Atomic and Molecular Gasmentioning
confidence: 62%
“…In addition to the inferred H2 fractions, observations have directly detected molecules in diffuse molecular clouds in absorption e.g., HCO + , HCN (Hogerheijde et al 1995a, HF, H2O (Flagey et al 2013, Sonnentrucker et al 2015, OH + , H2O + (e.g., Wyrowski et al 2010, Gerin et al 2010, ArH + (Schilke et al 2014, Jacob et al 2020, CH Sheffer et al (2008), SH Neufeld et al (2015), and in both absorption and emission e.g., OH , Busch et al 2019, with CH, HF and H2O being particularly good (linear) tracers of the H2 fraction. Although not strictly CO-dark in the original sense since the bulk of the gas may be detectable in H I, nevertheless these observations detect a portion of molecular gas that is not seen in CO emission.…”
Section: Diffuse Gasmentioning
confidence: 99%
“…This excess molecular gas points to the inability of CO to act as a proxy for H 2 , in regions of low dust column densities (or visual extinction) where CO readily undergoes photodissociation. In recent years, through observations of their radio and FIR rotational transitions, hydrides such as CH (Gerin et al 2010a;Wiesemeyer et al 2018;Jacob et al 2019), OH (Allen et al 2015;Engelke & Allen 2018;Rugel et al 2018;Busch et al 2019Busch et al , 2021 and HF (Neufeld et al 2010b;Sonnentrucker et al 2015) have been established as important tracers of CO-dark H 2 gas in addition to the [C II] 158 µm line (Langer et al 2014) and the J = 1 − 0 rotational transition of HCO + (Lucas & Liszt 1996;Gerin et al 2010b). We note that the CH-H 2 relationship was first established by Federman (1982) and later by Sheffer et al (2008) and then Weselak (2019) using optical observations of the A 2 ∆ -X 2 Π system of CH at 4300 Å and the (2−0), (3−0), and (4−0) bands of the Lyman B-X transitions of H 2 toward stars located in the local diffuse ISM (10 19 < N (H 2 ) < 10 21 cm −2 ).…”
Section: Hygal: Key Science Goalsmentioning
confidence: 99%