FOREST unbiased Galactic plane imaging survey with the Nobeyama 45 m telescope (FUGIN). VII. Molecular fraction of H i clouds

Author:

Nakanishi Hiroyuki1,Fujita Shinji2ORCID,Tachihara Kengo2,Izumi Natsuko3,Matsuo Mitsuhiro4,Umemoto Tomofumi4,Oasa Yumiko5,Inoue Tsuyoshi2

Affiliation:

1. Graduate School of Science and Engineering, Kagoshima University, 1-21-35 Korimoto, Kagoshima, Kagoshima 890-0065, Japan

2. Department of Physics, Nagoya University, Furo-cho, Chikusa-ku, Nagoya, Aichi 464-8602, Japan

3. College of Science, Ibaraki University, 2-1-1 Bunkyo, Mito, Ibaraki 310-8512, Japan

4. Nobeyama Radio Observatory, National Astronomical Observatory of Japan, National Institutes of Natural Sciences, 462-2 Nobeyama Minamimaki, Minamisaku, Nagano 384-1305, Japan

5. Faculty of Education, Saitama University, 255 Shimo-Okubo, Sakura-ku, Saitama, Saitama 338-8570, Japan

Abstract

ABSTRACT We analyze molecular-gas formation in neutral atomic hydrogen (H i) clouds using the latest CO data, obtained from the FOREST (four-beam receiver system on the 45 m telescope) unbiased Galactic plane imaging survey with the Nobeyama 45 m telescope, and using H i data taken from the Very Large Array Galactic plane survey. We applied a dendrogram algorithm to the H i data cube to identify H i clouds, and we calculated the H i mass and molecular-gas mass by summing the CO line intensity within each H i cloud. On the basis of the results, we created a catalog of 5737 identified H i clouds with local standard of rest (LSR) velocity of VLSR ≤ −20 km s−1 in galactic longitude and latitude ranges of 20° ≤ l ≤ 50° and −1° ≤ b ≤ 1°, respectively. We found that most of the H i clouds are distributed within a Galactocentric distance of 16 kpc, and most of them are in the cold neutral medium phase. In addition, we determined that the high-mass end of the H i mass function is fitted well with a power-law function with an index of 2.3. Although two sequences of self-gravitating and diffuse clouds are expected to appear in the M tot–$M_{\,{\rm H}_2}$ diagram according to previous works based on a plane-parallel model, the observational data show only a single sequence with large scattering within these two sequences. This implies that most of the clouds are mixtures of these two types of clouds. Moreover, we suggest the following scenario of molecular-gas formation: an H i-dominant cloud evolved with increasing H2 mass along a path of $M_{\,{\rm H}_2} \propto M_{\,\rm tot}^2$ by collecting diffuse gas before reaching and moving along the curves of the two sequences.

Funder

Nobeyama radio observatory

KAKENHI

National Radio Astronomy Observatory

National Science Foundation

Publisher

Oxford University Press (OUP)

Subject

Space and Planetary Science,Astronomy and Astrophysics

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1. A Catalog of 13CO Clumps from the MWISP in l = 10°–20°;Research in Astronomy and Astrophysics;2024-05-01

2. Semi-supervised deep learning for molecular clump verification;Astronomy & Astrophysics;2023-12-21

3. Ammonia mapping observations of the Galactic infrared bubble N49: Three NH3 clumps along the molecular filament;Publications of the Astronomical Society of Japan;2023-02-22

4. Molecular fraction in the Galactic Centre: The Central Molecular and H i Zones;Monthly Notices of the Royal Astronomical Society;2022-09-02

5. The “Maggie” filament: Physical properties of a giant atomic cloud;Astronomy & Astrophysics;2021-12-20

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