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LYRA ultra-faints: The emergence of faint dwarf galaxies in the presence of an early Lyman-Werner background

Published 26 Nov 2025 in astro-ph.GA and astro-ph.CO | (2511.21824v1)

Abstract: We present a suite of zoom-in cosmological hydrodynamical simulations of dwarf galaxies using the LYRA galaxy formation model with an extremely high mass resolution of 4 M⊙4\, \mathrm{M_{\odot}}, evolved to z=0z=0. The suite contains 65 haloes selected from Local Group like environments, spanning M200c=10<sup>7M_{\mathrm{200c}}=10<sup>7 to 5×10<sup>9 </sup>M⊙5\times10<sup>9\,</sup> \mathrm{M_{\odot}}. The sample includes small ultra-faints with M∗∼100 M⊙M_\ast\sim100\, \mathrm{M_{\odot}} through to classical dwarfs with M∗∼5×10<sup>6</sup>M⊙M_\ast \sim 5\times10<sup>6</sup> \mathrm{M_{\odot}}, as well as haloes that remain dark to the present day. We explore two prescriptions for the high-redshift ($z&gt;7$) Lyman-Werner background (LWB), differing in intensity and redshift evolution. Star formation begins early (z≳8z\gtrsim8) in progenitors with M200c∼10<sup>5M_{\mathrm{200c}}\sim10<sup>5-10<sup>6</sup></sup>M⊙10<sup>6</sup></sup> \mathrm{M_{\odot}}, where molecular hydrogen enables warm moderate-density gas to efficiently cool. The LWB strongly influences the z=0z=0 halo occupation fraction, shifting the dark-to-luminous transition from M200c∼10<sup>7</sup>M⊙M_{\mathrm{200c}}\sim10<sup>7</sup> \mathrm{M_{\odot}} (weaker LWB) to M200c∼10<sup>8</sup>M⊙M_{\mathrm{200c}}\sim10<sup>8</sup> \mathrm{M_{\odot}} (stronger LWB). Galaxies with M∗≳10<sup>5</sup>M⊙M_\ast\gtrsim10<sup>5</sup> \mathrm{M_{\odot}} are mostly insensitive to the LWB choice, whereas lower mass systems respond strongly, producing markedly different stellar mass-halo mass (SMHM) relations. The weaker LWB yields a very shallow SMHM slope with nearly constant scatter, while the stronger LWB introduces a pronounced break at M200c∼10<sup>9</sup>M⊙M_{\mathrm{200c}}\sim10<sup>9</sup> \mathrm{M_{\odot}}, where haloes of similar mass host galaxies with M∗∼10<sup>3M_\ast\sim10<sup>3 to 10<sup>5</sup>M⊙10<sup>5</sup> \mathrm{M_{\odot}} or remain dark. Both models produce a minimum stellar mass floor at M∗∼10<sup>3</sup>M⊙M_\ast\sim10<sup>3</sup> \mathrm{M_{\odot}}, originating from galaxies that undergo a single burst of star formation at high redshift before self-quenching from their first supernovae.

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