A comparison of \${\textbackslash}text\{{H}\}_2\$ formation models at high redshift. Schäbe, A., Romano-Díaz, E., Porciani, C., Ludlow, A. D., & Tomassetti, M. arXiv e-prints, 2003:arXiv:2003.04329, March, 2020.
A comparison of \${\textbackslash}text\{{H}\}_2\$ formation models at high redshift [link]Paper  abstract   bibtex   
Modelling the molecular gas that is routinely detected through CO observations of high-redshift galaxies constitutes a major challenge for ab initio simulations of galaxy formation. We carry out a suite of cosmological hydrodynamic simulations in order to compare three approximate methods that have been used in the literature to track the formation and evolution of the simplest and most abundant molecule, H\$_2\$. Namely, we consider: i) a semi-empirical procedure that associates H\$_2\$ to dark-matter haloes based on a series of scaling relations inferred from observations; ii) a model that assumes chemical equilibrium between the H\$_2\$ formation and destruction rates; and iii) a model that fully solves the out-of-equilibrium rate equations and accounts for the unresolved structure of molecular clouds. We study the impact of finite spatial resolution and show that robust H\$_2\$ masses at redshift \$z{\textbackslash}approx 4\$ can only be obtained for galaxies that are sufficiently metal enriched in which H\$_2\$ formation is fast. This corresponds to H\$_2\$ reservoirs with masses \$M_\{{\textbackslash}mathrm\{H_2\}\}{\textbackslash}gtrsim 6{\textbackslash}times 10{\textasciicircum}9 {\textbackslash}mathrm\{M\}_{\textbackslash}odot\$. In this range, equilibrium and non-equilibrium models predict similar molecular masses (but different galaxy morphologies) while the semi-empirical method produces less H\$_2\$. The star-formation rates as well as the stellar and H\$_2\$ masses of the simulated galaxies are in line with those observed in actual galaxies at similar redshifts that are not massive starbursts. The H\$_2\$ mass functions extracted from the simulations at \$z{\textbackslash}approx 4\$ agree well with recent observations that only sample the high-mass end. However, our results indicate that most molecular material at high-\$z\$ lies yet undetected in reservoirs with \$10{\textasciicircum}9
@article{schabe_comparison_2020,
	title = {A comparison of \${\textbackslash}text\{{H}\}\_2\$ formation models at high redshift},
	volume = {2003},
	url = {http://adsabs.harvard.edu/abs/2020arXiv200304329S},
	abstract = {Modelling the molecular gas that is routinely detected through CO observations of high-redshift galaxies constitutes a major challenge for ab initio simulations of galaxy formation. We carry out a suite of cosmological hydrodynamic simulations in order to compare three
approximate methods that have been used in the literature to track the formation and evolution of the simplest and most abundant molecule, H\$\_2\$. Namely, we consider: i) a semi-empirical procedure that
associates H\$\_2\$ to dark-matter haloes based on a series of scaling relations inferred from observations; ii) a model that assumes chemical equilibrium between the H\$\_2\$ formation and destruction rates; and iii) a model that fully solves the out-of-equilibrium rate equations and accounts for the unresolved structure of molecular clouds. We study the impact of finite spatial resolution and show that robust H\$\_2\$ masses at redshift \$z{\textbackslash}approx 4\$ can only be obtained for galaxies that are sufficiently metal enriched in which H\$\_2\$ formation is fast. This corresponds to H\$\_2\$ reservoirs with masses \$M\_\{{\textbackslash}mathrm\{H\_2\}\}{\textbackslash}gtrsim 6{\textbackslash}times 10{\textasciicircum}9 {\textbackslash}mathrm\{M\}\_{\textbackslash}odot\$. In this range, equilibrium and
non-equilibrium models predict similar molecular masses (but different galaxy morphologies) while the semi-empirical method produces less H\$\_2\$. The star-formation rates as well as the stellar and H\$\_2\$ masses of the simulated galaxies are in line with those observed in actual galaxies at similar redshifts that are not massive starbursts. The H\$\_2\$ mass functions extracted from the simulations at \$z{\textbackslash}approx 4\$ agree well with recent observations that only sample the high-mass end. However, our results indicate that most molecular material at high-\$z\$ lies yet undetected in reservoirs with \$10{\textasciicircum}9},
	urldate = {2020-03-12},
	journal = {arXiv e-prints},
	author = {Schäbe, Alexander and Romano-Díaz, Emilio and Porciani, Cristiano and Ludlow, Aaron D. and Tomassetti, Matteo},
	month = mar,
	year = {2020},
	keywords = {Astrophysics - Astrophysics of Galaxies},
	pages = {arXiv:2003.04329},
}

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