Astraeus X: Indications of a top-heavy initial mass function in highly star-forming galaxies from JWST observations at z>10

TL;DR

This study introduces an evolving, top-heavy initial mass function (IMF) model in galaxy simulations, which successfully explains the abundance of bright UV galaxies at redshifts greater than 10 observed by JWST, and impacts reionisation history.

Contribution

It presents a novel evolving IMF model that becomes increasingly top-heavy with gas density, improving the match to high-redshift galaxy observations and reionisation predictions.

Findings

Reproduces observed UV luminosity functions at z=5-15.

Enhances UV brightness in massive galaxies by up to 2.6 magnitudes.

Predicts earlier reionisation with larger ionised regions.

Abstract

The James Webb Space Telescope (JWST) has uncovered an abundance of $z>10$ galaxies bright in the ultraviolet (UV) that has challenged traditional theoretical models at high redshifts. Recently, various new models have emerged to address this discrepancy by refining their description of star formation. Here we investigate whether modifications to the stellar initial mass function (IMF) alone can reproduce the $z>10$ UV luminosity functions (UV LFs) when the star formation rate is used as a proxy for the fraction of massive stars. We incorporate an Evolving IMF into the {\sc astraeus} galaxy evolution and reionisation simulation framework, which becomes increasingly top-heavy as the gas density in a galaxy rises above a given threshold. Our implementation accounts for the IMF's effects on supernova (SN) feedback, metal enrichment, and the UV and ionising emissivities. For this Evolving IMF model, we find that (i) the maximum UV luminosity enhancement is twice as large in massive galaxies ($\Delta M_\mathrm{UV}\simeq2.6$) than those where star formation is strongly limited by SN feedback ($\Delta M_\mathrm{UV}\simeq1.3$); (ii) it successfully reproduces the observed UV LFs at $z=5-15$; (iii) galaxies with top-heavy IMFs exhibit the highest star formation rates, driven by their location in local density peaks, which facilitates higher gas accretion rates; (iv) the $1\sigma$ variances in the UV luminosity are only slightly higher compared to when assuming a Salpeter IMF, but the $2\sigma$ variances are significantly increased by a factor of $1.4-2$ boosting the abundance of UV-bright galaxies at $z>10$; (v) reionisation begins earlier with more extended large ionised regions and fewer smaller ones during its initial stages, though these differences diminish at lower redshifts, leading to a similar end of reionisation at $z\simeq5.6$.}