The production and escape of Lyman-Continuum radiation from star-forming galaxies at z~2 and their redshift evolution

TL;DR

This study measures the ionizing photon escape fraction from star-forming galaxies at z~2, finding low escape fractions but a significant increase in ionizing photon production efficiency with redshift, informing reionization models.

Contribution

It provides new measurements of escape fractions and ionizing photon production efficiency at z~2, and explores their evolution up to higher redshifts, improving understanding of galaxy contributions to reionization.

Findings

Escape fraction f_esc < 2.8-6.4% at z=2.2

Ionizing photon production efficiency ξ_ion increases with redshift

ξ_ion ≈ 10^{25.4} Hz erg^{-1} in the reionization era

Abstract

We study the production rate of ionizing photons of a sample of 588 H$\alpha$ emitters (HAEs) and 160 Lyman-$\alpha$ emitters (LAEs) at $z=2.2$ in the COSMOS field in order to assess the implied emissivity from galaxies, based on their UV luminosity. By exploring the rest-frame Lyman Continuum (LyC) with GALEX/$NUV$ data, we find f$_{\rm esc} < 2.8\, (6.4)$% through median (mean) stacking. By combining the H$\alpha$ luminosity density with IGM emissivity measurements from absorption studies, we find a globally averaged $\langle$f$_{\rm esc}\rangle$ of $5.9^{+14.5}_{-4.2}$ % at $z=2.2$ if we assume HAEs are the only source of ionizing photons. We find similarly low values of the global $\langle$f$_{\rm esc}\rangle$ at $z\approx3-5$, also ruling out a high $\langle$f$_{\rm esc}\rangle$ at $z<5$. These low escape fractions allow us to measure $\xi_{ion}$, the number of produced ionizing photons per unit UV luminosity, and investigate how this depends on galaxy properties. We find a typical $\xi_{ion} \approx 10^{24.77\pm0.04}$ Hz erg$^{-1}$ for HAEs and $\xi_{ion} \approx 10^{25.14\pm0.09}$ Hz erg$^{-1}$ for LAEs. LAEs and low mass HAEs at $z=2.2$ show similar values of $\xi_{ion}$ as typically assumed in the reionization era, while the typical HAE is three times less ionizing. Due to an increasing $\xi_{ion}$ with increasing EW(H$\alpha$), $\xi_{ion}$ likely increases with redshift. This evolution alone is fully in line with the observed evolution of $\xi_{ion}$ between $z\approx2-5$, indicating a typical value of $\xi_{ion} \approx 10^{25.4}$ Hz erg$^{-1}$ in the reionization era.