Dissecting Reionisation with the Cosmic Star Formation and Active Galactic Nuclei Luminosity History
Jordan C. J. D'Silva, Simon P. Driver, Claudia D. P. Lagos, Aaron S. G. Robotham, Nathan J. Adams, Christopher J. Conselice, Brenda Frye, Nimish P. Hathi, Thomas Harvey, Anton M. Koekemoer, Rafael Ortiz, Massimo Ricotti, Clayton Robertson, Ross M. Silver, Stephen M. Wilkins, Christopher N. A. Willmer, Rogier A. Windhorst, Seth H. Cohen, Rolf A. Jansen, Jake Summers, Dan Coe, Norman A. Grogin, Madeline A. Marshall, Nor Pirzkal, Russell E. Ryan, Haojing Yan
TL;DR
This work connects the cosmic star formation history (CSFH) and cosmic AGN luminosity history (CAGNH) to the cosmic spectral energy distribution (CSED) using the ProSpect SED model to study reionisation. By bracketing the ionising emissivity with escape fractions for both stars and AGN, it shows that stellar photons could reionise the IGM by $z\approx6$ if $f_{\mathrm{esc}}$ is sufficiently large (roughly $10-30\%$ depending on metallicity), while AGN alone are unlikely to achieve this even at $f_{\mathrm{esc}}=1$. A hybrid model with $f_{\mathrm{esc}}^{\mathrm{stars}}\approx12\%$ and $f_{\mathrm{esc}}^{\mathrm{AGN}}\approx63\%$ provides a consistent reionisation history, reconciling the CSFH/CAGNH with the Planck $\tau_{\mathrm{CMB}}$ and Gunn-Peterson constraints. The analysis emphasizes that stars likely dominated early reionisation but AGN played a non-negligible role in sustaining ionisation at $z\lesssim6$, while highlighting systematic uncertainties in escape fractions and the clumping factor $\mathcal{C}$ as key limitations for precise inferences.
Abstract
The combination of the $z=0-13.5$ cosmic star formation history and active galactic nuclei (AGN) luminosity history as inferred by the James Webb Space Telescope is connected to the cosmic spectral energy distribution (CSED) to explore the sources of reionisation. We compute the redshift evolution of the corresponding cosmic ionising photon emissivity, the neutral fraction and the cosmic microwave background optical depth. We use the generative SED modelling code ProSpect to bracket the ionising emissivity between escape fractions of $f_{\mathrm{esc}} = 1 - 100\%$ for both the stars and AGN. Stars alone could have achieved reionisation by $z\approx 6$ with $f_{\mathrm{esc}} \gtrsim 30\%$ for solar metallicity ($Z=0.02$) stars or $f_{\mathrm{esc}} \gtrsim 10\%$ for metal-poor ($Z=10^{-4}$) stars. On the other hand, AGN by themselves would have struggled to produce sufficiently many ionising photons even with $f_{\mathrm{esc}} = 100\%$. A hybrid model containing both stars and AGN is explored where we find best fit (median$\pm 1σ$) $f_{\mathrm{esc}}=$ $12\%$ ($14^{+9}_{-7}\%$) for the stars and $f_{\mathrm{esc}}=$ $63\%$ ($60^{+28}_{-32}\%$) for the AGN, maintained at all redshifts. In essence, the joint growth of stellar mass and supermassive black holes produces neither more nor fewer ionising photons than needed to reionise $\gtrsim 99\%$ of the intergalactic medium by $z\approx 6$.
