2025MNRAS.543.2507F


Query : 2025MNRAS.543.2507F

2025MNRAS.543.2507F - Mon. Not. R. Astron. Soc., 543, 2507-2522 (2025/November-1)

Pressure-regulated formation of molecular clouds and stars: the case of the Milky Way.

FRANCO J., RODRIGUEZ-PUEBLA A., BALLESTEROS-PAREDES J. and ZAMORA-AVILEZ M.

Abstract (from CDS):

We present a steady-state analytical model for pressure-regulated formation of molecular clouds (MC) and stars in gaseous galactic discs and apply it to the Milky Way (MW). MC formation depends on mid-plane interstellar pressure $P_{\mathrm{ISM}}$ and metallicity Z, and for galactocentric distances $R\gtrsim 5$ kpc, $P_{\mathrm{ISM}}(R)$ scales approximately linearly with molecular gas surface density $\Sigma _{\rm mol}(R)$. The molecularization of the cold neutral medium (CNM) is due to the opacity of small dust grains that protect the centre of the cloud from dissociating radiation when the column density is $\Sigma _{\rm d}\ge 5 ({\rm Z}_\odot/Z) \, {\rm M}_\odot \, \text{pc}^{-2}$. The H$_2$ formation rate per hydrogen atom is $F\sim 10^{-15} (P_{\mathrm{ISM}}/{\rm P}_\odot)T_{100}^{-1/2} \, \text{s}^{-1}$, and the corresponding formation rate per unit area is $\dot{\Sigma }^{+}_{\rm mol}\sim 5 \times 10^{-2}\left(P_{\mathrm{ISM}}/{{\rm P}_\odot }\right)T_{100}^{-1/2} \, {\rm M}_\odot \, \text{kpc}^{-2} \, \text{yr}^{-1}$, where ${\rm P}_\odot$ is the pressure at the solar circle and $T_{100}=T/100 \, \text{K}$ is the temperature of the cloud. In equilibrium, this equals the molecular gas destruction rate $\dot{\Sigma }^{-}_{\rm mol}$ due to star formation. Self-gravity sets in when the column density of a cloud reaches $\Sigma _{\rm sg}=\Sigma _{\rm sg,\odot }(P_{\mathrm{ISM}}/{\rm P}_\odot)^{1/2}$, with $\Sigma _{\rm sg,\odot }\sim 30\, {\rm M}_\odot \, \text{pc}^{-2}$. Given the distribution of $P_{\mathrm{ISM}}(R)$ and $Z(R)$ in the MW, the star formation process at $5\lesssim R\lesssim 11$ kpc follows a two-step track: first, MCs form from CNM gas and then they form stars when self-gravity sets in. The resulting star formation rate surface density is $\Sigma _\text{SFR}(R)\approx (1.6\!-\!4)\times 10^{-3}\left(P_{\mathrm{ISM}}/{\rm P}_\odot \right)\, \text{M}_\odot \, \text{kpc}^{-2} \, \text{yr}^{-1}$ with an average final star formation efficiency of $\epsilon _{\rm sf}\sim (3\!-\!8)\times 10^{-2}$.

Abstract Copyright: © The Author(s) 2025. Published by Oxford University Press on behalf of Royal Astronomical Society.

Journal keyword(s): ISM: clouds - H ii regions - local interstellar matter - galaxies: star formation

Simbad objects: 7

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Number of rows : 7
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 M 31 AGN 00 42 44.330 +41 16 07.50 4.86 4.36 3.44     ~ 13622 1
2 IC 1613 GiC 01 04 48.4071 +02 07 10.185   10.42 10.01 9.77   ~ 1316 2
3 M 33 GiG 01 33 50.8965749232 +30 39 36.630403128 6.17 6.27 5.72     ~ 6226 1
4 NAME Magellanic Clouds GrG 03 00 -71.0           ~ 7988 0
5 MCG-01-26-030 H2G 10 11 00.5 -04 41 30 12.48 12.13 11.93 11.78   ~ 789 2
6 NAME Galactic Center reg 17 45 39.60213 -29 00 22.0000           ~ 16269 0
7 NAME Local Group GrG ~ ~           ~ 9325 0

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