The THESAN-ZOOM project: Star-formation efficiencies in high-redshift galaxies

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Main Authors: Shen, Xuejian, Kannan, Rahul, Puchwein, Ewald, Smith, Aaron, Vogelsberger, Mark, Borrow, Josh, Garaldi, Enrico, Keating, Laura, Zier, Oliver, McClymont, William, Tacchella, Sandro, Wang, Zihao, Hernquist, Lars
Format: Preprint
Published: 2025
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author Shen, Xuejian
Kannan, Rahul
Puchwein, Ewald
Smith, Aaron
Vogelsberger, Mark
Borrow, Josh
Garaldi, Enrico
Keating, Laura
Zier, Oliver
McClymont, William
Tacchella, Sandro
Wang, Zihao
Hernquist, Lars
author_facet Shen, Xuejian
Kannan, Rahul
Puchwein, Ewald
Smith, Aaron
Vogelsberger, Mark
Borrow, Josh
Garaldi, Enrico
Keating, Laura
Zier, Oliver
McClymont, William
Tacchella, Sandro
Wang, Zihao
Hernquist, Lars
contents Recent JWST observations hint at unexpectedly intense cosmic star-formation in the early Universe, often attributed to enhanced star-formation efficiencies (SFEs). Here, we analyze the SFE in THESAN-ZOOM, a novel zoom-in radiation-hydrodynamic simulation campaign of high-redshift ($z \gtrsim 3$) galaxies employing a state-of-the-art galaxy formation model resolving the multiphase interstellar medium (ISM). The halo-scale SFE ($ε^{\ast}_{\rm halo}$) - the fraction of baryons accreted by a halo that are converted to stars - follows a double power-law dependence on halo mass, with a mild redshift evolution above $M_{\rm halo} \gtrsim 10^{9.5}\,{\rm M}_{\odot}$. The power-law slope is roughly $1/3$ at large halo masses, consistent with expectations when gas outflows are momentum-driven. At lower masses, the slope is roughly $2/3$ and is more aligned with the energy-driven outflow scenario. $ε^{\ast}_{\rm halo}$ is a factor of $2-3$ larger than commonly assumed in empirical galaxy-formation models at $M_{\rm halo} \lesssim 10^{11}\,{\rm M}_{\odot}$. On galactic (kpc) scales, the Kennicutt-Schmidt (KS) relation of neutral gas is universal in THESAN-ZOOM, following $Σ_{\rm SFR} \propto Σ_{\rm gas}^2$, indicative of a turbulent energy balance in the ISM maintained by stellar feedback. The rise of $ε^{\ast}_{\rm halo}$ with halo mass can be traced primarily to increasing gas surface densities in massive galaxies, while the underlying KS relation and neutral, star-forming gas fraction remain unchanged. Although the increase in $ε^{\ast}_{\rm halo}$ with redshift is relatively modest, it is sufficient to explain the large observed number density of UV-bright galaxies at $z \gtrsim 12$. However, reproducing the brightest sources at $M_{\rm UV} \lesssim -21$ may require extrapolating the SFE beyond the halo mass range directly covered by THESAN-ZOOM.
format Preprint
id arxiv_https___arxiv_org_abs_2503_01949
institution arXiv
publishDate 2025
record_format arxiv
spellingShingle The THESAN-ZOOM project: Star-formation efficiencies in high-redshift galaxies
Shen, Xuejian
Kannan, Rahul
Puchwein, Ewald
Smith, Aaron
Vogelsberger, Mark
Borrow, Josh
Garaldi, Enrico
Keating, Laura
Zier, Oliver
McClymont, William
Tacchella, Sandro
Wang, Zihao
Hernquist, Lars
Astrophysics of Galaxies
Cosmology and Nongalactic Astrophysics
Recent JWST observations hint at unexpectedly intense cosmic star-formation in the early Universe, often attributed to enhanced star-formation efficiencies (SFEs). Here, we analyze the SFE in THESAN-ZOOM, a novel zoom-in radiation-hydrodynamic simulation campaign of high-redshift ($z \gtrsim 3$) galaxies employing a state-of-the-art galaxy formation model resolving the multiphase interstellar medium (ISM). The halo-scale SFE ($ε^{\ast}_{\rm halo}$) - the fraction of baryons accreted by a halo that are converted to stars - follows a double power-law dependence on halo mass, with a mild redshift evolution above $M_{\rm halo} \gtrsim 10^{9.5}\,{\rm M}_{\odot}$. The power-law slope is roughly $1/3$ at large halo masses, consistent with expectations when gas outflows are momentum-driven. At lower masses, the slope is roughly $2/3$ and is more aligned with the energy-driven outflow scenario. $ε^{\ast}_{\rm halo}$ is a factor of $2-3$ larger than commonly assumed in empirical galaxy-formation models at $M_{\rm halo} \lesssim 10^{11}\,{\rm M}_{\odot}$. On galactic (kpc) scales, the Kennicutt-Schmidt (KS) relation of neutral gas is universal in THESAN-ZOOM, following $Σ_{\rm SFR} \propto Σ_{\rm gas}^2$, indicative of a turbulent energy balance in the ISM maintained by stellar feedback. The rise of $ε^{\ast}_{\rm halo}$ with halo mass can be traced primarily to increasing gas surface densities in massive galaxies, while the underlying KS relation and neutral, star-forming gas fraction remain unchanged. Although the increase in $ε^{\ast}_{\rm halo}$ with redshift is relatively modest, it is sufficient to explain the large observed number density of UV-bright galaxies at $z \gtrsim 12$. However, reproducing the brightest sources at $M_{\rm UV} \lesssim -21$ may require extrapolating the SFE beyond the halo mass range directly covered by THESAN-ZOOM.
title The THESAN-ZOOM project: Star-formation efficiencies in high-redshift galaxies
topic Astrophysics of Galaxies
Cosmology and Nongalactic Astrophysics
url https://arxiv.org/abs/2503.01949