Steep Redshift Evolution of the Ionizing Escape Fraction at z = 5--12: Empirical Constraints and Comparison with Simulations

Abstract

The ionizing photon escape fraction f esc governs cosmic reionization yet remains observationally unconstrained as a function of halo mass. We present the first empirical constraints on f esc(M h,z) across the epoch of reionization, using a three-parameter power-law model f esc = f0\,(M/1010M)αM\,[(1+z)/10]αz, conditioned on HST and JWST UV luminosity functions at z=5--12, the Planck Thomson optical depth, seven neutral-fraction measurements, and one high-redshift prior. Using Schechter fits to the latest HST and JWST UV luminosity functions, abundance matching to link M UV to halo mass, and a reionization ODE solver validated against Planck, we constrain the model via a dense grid scan and ensemble MCMC. The profile likelihood yields tight constraints: f0=0.061-0.023+0.018, αM=0.18-0.30+0.22, αz=1.98-0.42+0.48. In contrast, the full marginal posterior is substantially broadened by a strong f0--αM--αz degeneracy (αz = 1.93-2.00+2.09, αM = -0.52-0.69+0.69). The population-averaged f esc (z) rises from 2\% at z=5 to 9\% at z=12, with sub-threshold halos contributing >80\% of the ionizing budget at z≥10. Comparing with THESAN, we find that the per-halo median f esc shows steep evolution consistent with our profile result, while luminosity-weighted averaging systematically flattens the trend because massive halos dominate the ionizing budget at z7. Robustness checks confirm αz>1.0 at >95\% confidence; the steep-evolution model predicts τe=0.047, consistent with Planck at 0.7σ. We provide tabulated f esc(M h,z) posteriors as empirical inputs for reionization simulations.

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