TY - JOUR
T1 - Nature of Supersonic Turbulence and Density Distribution Function in the Multiphase Interstellar Medium
AU - Kobayashi, Masato I.N.
AU - Inoue, Tsuyoshi
AU - Tomida, Kengo
AU - Iwasaki, Kazunari
AU - Nakatsugawa, Hiroki
N1 - Funding Information:
We are grateful to the anonymous reviewer for careful reading and comments, which improved our manuscript significantly. Numerical computations were carried out on Cray XC30 and XC50 at the Center for Computational Astrophysics, National Astronomical Observatory of Japan. M.I.N.K. (15J04974, 18J00508, 20H04739), T.I. (18H05436, 20H01944), K.T. (16H05998, 16K13786, 17KK0091, 21H04487), and K.I. (19K03929, 19H01938), are supported by Grants-in-Aid from the Ministry of Education, Culture, Sports, Science, and Technology of Japan. M.I.N.K. appreciates Atsushi J. Nishizawa and Chiaki Hikage for helping our Fourier analysis. M.I.N.K. is grateful to Tomoaki Matsumoto, Kazuyuki Omukai, Hajime Susa, Sho Higashi, Gen Chiaki, Hajime Fukushima, Shu-ichiro Inutsuka, Shinsuke Takasao, Tetsuo Hasegawa, and Kengo Tachihara for fruitful comments. We are grateful to Hiroki Nakatsugawa, who contributed to the early phase of this study through his master thesis work.
Publisher Copyright:
© 2022. The Author(s). Published by the American Astronomical Society.
PY - 2022/5/1
Y1 - 2022/5/1
N2 - Supersonic flows in the interstellar medium (ISM) are believed to be a key driver of the molecular cloud formation and evolution. Among molecular clouds' properties, the ratio between the solenoidal and compressive modes of turbulence plays important roles in determining the star formation efficiency. We use numerical simulations of supersonic converging flows of the warm neutral medium (WNM) resolving the thermal instability to calculate the early phase of molecular cloud formation, and we investigate the turbulence structure and the density probability distribution function (density PDF) of the multiphase ISM. We find that both the solenoidal and compressive modes have their power spectrum similar to the Kolmogorov spectrum. The solenoidal (compressive) modes account for ≳80% (≲20%) of the total turbulence power. When we consider both the cold neutral medium (CNM) and the thermally unstable neutral medium (UNM) up to T ≲ 400 K, the density PDF follows the lognormal distribution, whose width σs is well explained by the known relation from the isothermal turbulence as σs=ln(1+b2M2) (where b is the parameter representing the turbulence mode ratio and M is the turbulent Mach number). The density PDF of the CNM component alone (T ≤ 50 K), however, exhibits a narrower σs by a factor of ∼2. These results suggest that observational estimations of b based on the CNM density PDF requires the internal turbulence within each CNM clump but not the interclump relative velocity, the latter of which is instead powered by the WNM/UNM turbulence.
AB - Supersonic flows in the interstellar medium (ISM) are believed to be a key driver of the molecular cloud formation and evolution. Among molecular clouds' properties, the ratio between the solenoidal and compressive modes of turbulence plays important roles in determining the star formation efficiency. We use numerical simulations of supersonic converging flows of the warm neutral medium (WNM) resolving the thermal instability to calculate the early phase of molecular cloud formation, and we investigate the turbulence structure and the density probability distribution function (density PDF) of the multiphase ISM. We find that both the solenoidal and compressive modes have their power spectrum similar to the Kolmogorov spectrum. The solenoidal (compressive) modes account for ≳80% (≲20%) of the total turbulence power. When we consider both the cold neutral medium (CNM) and the thermally unstable neutral medium (UNM) up to T ≲ 400 K, the density PDF follows the lognormal distribution, whose width σs is well explained by the known relation from the isothermal turbulence as σs=ln(1+b2M2) (where b is the parameter representing the turbulence mode ratio and M is the turbulent Mach number). The density PDF of the CNM component alone (T ≤ 50 K), however, exhibits a narrower σs by a factor of ∼2. These results suggest that observational estimations of b based on the CNM density PDF requires the internal turbulence within each CNM clump but not the interclump relative velocity, the latter of which is instead powered by the WNM/UNM turbulence.
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U2 - 10.3847/1538-4357/ac5a54
DO - 10.3847/1538-4357/ac5a54
M3 - Article
AN - SCOPUS:85130116331
SN - 0004-637X
VL - 930
JO - Astrophysical Journal
JF - Astrophysical Journal
IS - 1
M1 - 76
ER -