ArXiv TLDR

The Critical Mass in Galaxy Evolution

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2604.27477

Preetish K. Mishra, Changbom Park, Jaehyun Lee, Yohan Dubois, Christophe Pichon + 2 more

astro-ph.GAastro-ph.CO

TLDR

This paper identifies a critical mass in galaxies where gas accretion changes, suppressing star formation and driving the stellar-to-total mass ratio turnover.

Key contributions

  • Identifies a redshift-independent critical mass at $M_{\rm tot} \sim 10^{12.5}{\rm M_\odot}$ in galaxy evolution.
  • This critical mass arises from a stable hot gas halo forming, suppressing cool gas inflow and star formation.
  • The stellar-to-total mass ratio (STR) evolution is primarily driven by changes in the stellar-to-baryon mass ratio.
  • A secondary critical mass at $M_{\rm tot} \approx 10^{11}{\rm M_\odot}$ marks where gas retention peaks.

Why it matters

This research clarifies the physical mechanisms behind the "critical mass" phenomenon in galaxy evolution, a key threshold where galaxy properties fundamentally change. Understanding how gas accretion and hot gas halos influence star formation efficiency at different mass scales is crucial for refining galaxy formation models.

Original Abstract

We investigate the physical origin of critical mass, a threshold where many galaxy properties and scaling relations undergo fundamental transitions, using the Horizon Run 5 simulation. Focusing on massive ($M_{\rm tot} \geq 10^{12}{\rm M_\odot}$) central galaxies, we examine the mass-dependent turnover of the stellar-to-total mass ratio (STR) and the physical processes driving it. We decompose STR into the stellar-to-baryon mass ratio ($M_*/M_{\rm bar}$) and baryon retention fraction ($M_{\rm bar}/M_{\rm tot}$) to examine galaxies' ability to retain baryons and convert them into stars. We find that STR evolution is dominated by variation in $M_*/M_{\rm bar}$, which changes by over a factor of three, peaking within a narrow range of $M_{\rm tot} \sim 10^{12.4\text{--}12.7}{\rm M_\odot}$ independent of redshift, while $M_{\rm bar}/M_{\rm tot}$ varies by at most 30%. A redshift-independent critical mass at $M_{\rm tot} \sim 10^{12.5}{\rm M_\odot}$ ($M_* \sim 10^{10.7}{\rm M_\odot}$) arises from the changing nature of gas accretion. At this scale, a dynamically stable hot gas halo develops that suppresses cool gas inflow, reducing in-situ star formation efficiency such that $M_{\rm tot}$ growth exceeds in-situ $M_{*}$ growth. Consequently, the hot gas reservoir grows while $M_{*}$ growth slows, producing upturns in $M_{\rm gas}/M_{\rm tot}$ and $M_{\rm bar}/M_{\rm tot}$ and a downturn in $M_{*}/M_{\rm bar}$ that ultimately drives the STR turnover. We also identify a secondary critical mass at $M_{\rm tot} \approx 10^{11}{\rm M_\odot}$ (or $M_{*} \approx 10^{9\text{--}9.5}{\rm M_\odot}$) where gas retention fraction peaks, above which increasing hot gas fraction gradually suppresses in-situ star formation efficiency.

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