Dust-Gas Scaling Relations and OH Abundance in the Galactic ISM

• Published in: The Astrophysical journal Vol. 862; no. 1; pp. 49 - 66
• Main Authors: Nguyen, Hiep, Dawson, J. R., Miville-Deschênes, M.-A., Tang, Ningyu, Li, Di, Heiles, Carl, Murray, Claire E., Stanimirovi, Sne ana, Gibson, Steven J., McClure-Griffiths, N. M., Troland, Thomas, Bronfman, L., Finger, R.
• Format: Journal Article
• Language: English
• Published: Philadelphia The American Astronomical Society 20.07.2018; IOP Publishing
• Subjects: Astrophysics; Cosmic dust; Density; Dust; Dust data; dust, extinction; Hydrogen; Interstellar dust; Interstellar gas; Interstellar matter; Interstellar medium; ISM: clouds; ISM: molecules; Molecular gases; Opacity; Optical analysis; Optical thickness
• ISSN: 0004-637X; 1538-4357
• DOI: 10.3847/1538-4357/aac82b

Observations of interstellar dust are often used as a proxy for total gas column density NH. By comparing Planck thermal dust data (Release 1.2) and new dust reddening maps from Pan-STARRS 1 and 2MASS, with accurate (opacity-corrected) H i column densities and newly published OH data from the Arecibo Millennium survey and 21-SPONGE, we confirm linear correlations between dust optical depth τ353, reddening E(B − V), and the total proton column density NH in the range (1-30) × 1020 cm−2, along sightlines with no molecular gas detections in emission. We derive an NH/E(B − V) ratio of (9.4 1.6) × 1021 cm−2 mag−1 for purely atomic sightlines at b > 5 ° , which is 60% higher than the canonical value of Bohlin et al. We report a ∼40% increase in opacity 353 = τ353/NH, when moving from the low column density (NH < 5 × 1020 cm−2) to the moderate column density (NH > 5 × 1020 cm−2) regime, and suggest that this rise is due to the evolution of dust grains in the atomic interstellar medium. Failure to account for H i opacity can cause an additional apparent rise in 353 of the order of a further ∼20%. We estimate molecular hydrogen column densities N H 2 from our derived linear relations, and hence derive the OH/H2 abundance ratio of XOH ∼ 1 × 10−7 for all molecular sightlines. Our results show no evidence of systematic trends in OH abundance with N H 2 in the range N H 2 ∼ (0.1−10) × 1021 cm−2. This suggests that OH may be used as a reliable proxy for H2 in this range, which includes sightlines with both CO-dark and CO-bright gas.