H ɪ, CO, and Planck/IRAS dust properties in the high latitude cloud complex, MBM 53, 54, 55 and HLCG 92-35. Possible evidence for an optically thick HI envelope around the CO clouds
posted on 2023-05-18, 05:56authored byFukui, Y, Okamoto, R, Kaji, R, Yamamoto, H, Torii, K, Hayakawa, T, Tachihara, K, John DickeyJohn Dickey, Okuda, T, Ohama, A, Kuroda, Y, Kuwahara, T
We present an analysis of the Hɪ and CO gas in conjunction with the <i>Planck/IRAS</i> submillimeter/far-infrared dust properties toward the most outstanding high latitude clouds MBM53, 54, 55 and HLCG 92 − 35 at <i>b</i> = −30° to−45°. The CO emission, dust opacity at 353 GHz (τ<sub>353</sub>), and dust temperature (<i>T</i><sub>d</sub>) show generally good spatial correspondence. On the other hand, the correspondence between the Hɪ emission and the dust properties is less clear than in CO. The integrated Hɪ intensity <i>W</i><sub>Hɪ</sub> and τ<sub>353</sub> show a large scatter with a correlation coefficient of ∼0.6 for a <i>T</i><sub>d</sub> range from 16K to 22K. We find, however, that <i>W</i><sub>Hɪ</sub> and τ<sub>353</sub> show better correlation for smaller ranges of <i>T</i><sub>d</sub> every 0.5K, generally with a correlation coefficient of 0.7–0.9.We set up a hypothesis that the Hɪ gas associated with the highest <i>T</i><sub>d</sub> ≥ 21.5K is optically thin, whereas the Hɪ emission is generally optically thick for <i>T</i><sub>d</sub> lower than 21.5K. We have determined a relationship for the optically thin Hɪ gas between atomic hydrogen column density and τ<sub>353</sub>, <i>N</i><sub>Hɪ</sub> (cm<sup>−2</sup>) = (1.5 × 10<sup>26</sup>)· τ<sub>353</sub>, under the assumption that the dust properties are uniform and we have applied this to estimate <i>N</i><sub>Hɪ</sub> from τ<sub>353</sub> for the whole cloud. <i>N</i><sub>Hɪ</sub> was then used to solve for <i>τ</i><sub>s</sub> and <i>N</i><sub>Hɪ</sub> over the region. The result shows that the Hɪ is dominated by optically thick gas having a low spin temperature of 20–40K and a density of 40–160 cm<sup>−3</sup>. The Hɪ envelope has a total mass of ∼1.2 × 10<sup>4</sup> <i>M</i><sub>☉</sub>, an order of magnitude larger than that of the CO clouds. The Hɪ envelope properties derived by this method do not rule out a mixture of Hɪ and H<sub>2</sub> in the dark gas, but we present indirect evidence that most of the gas mass is in the atomic state.