Metallicity-Dependent quenching of Star Formation at High Redshift in Small Galaxies

TL;DR

This study models how metallicity influences star formation suppression in small high-redshift galaxies, revealing that low metallicity limits star formation, leading to a dominance of ex situ growth and specific star formation rate trends.

Contribution

It introduces a simple model incorporating metallicity-dependent star formation, explaining suppression effects and the evolution of star formation and metallicity in small galaxies at high redshift.

Findings

Star formation is suppressed in low-metallicity, low-mass halos at z>2.

Ex situ star formation dominates in small galaxies at high redshift.

Predicted relations of sSFR and metallicity with stellar mass and redshift.

Abstract

[abridged] The star formation rates (SFR) of low-metallicity galaxies depend sensitively on the gas metallicity, because metals are crucial to mediating the transition from intermediate-temperature atomic gas to cold molecular gas, a necessary precursor to star formation. We study the impact of this effect on the star formation history of galaxies. We incorporate metallicity-dependent star formation and metal enrichment in a simple model that follows the evolution of a halo main progenitor. Our model shows that including the effect of metallicity leads to suppression of star formation at redshift z>2 in dark halos with masses <~ 10^11 Msun, with the suppression becoming near total for halos below ~10^9.5-10 Msun. We find that at high redshift the SFR cannot catch up with the gas inflow rate (IR), because the SFR is limited by the free-fall time, and because it is suppressed further by a lack of metals. As a result, in each galaxy the SFR is growing in time faster than the IR, and the integrated cosmic SFR density is rising with time. The suppressed in situ SFR at high z makes the growth of stellar mass dominated by ex situ SFR which implies that the specific SFR (sSFR) remains constant with time. The intensely accreted gas at high z is accumulating as an atomic gas reservoir. This provides additional fuel for star formation in 10^10 - 10^12 Msun halos at z ~ 1-3, which allows the SFR to exceed the instantaneous IR, and may enable an even higher outflow rate. At z<1, following the natural decline in IR with time due to the universal expansion, the SFR and sSFR are expected to drop. We specify the expected dependence of sSFR and metallicity on stellar mass and redshift. At a given z, and below a critical mass, these relations are predicted to be flat and rising respectively. Our model predictions qualitatively match some of the puzzling features in the observed star formation history.