Abstract

We present a new modeling of the X-ray luminosity function (XLF) of Active Galactic Nuclei (AGN) out to z∼\sim3, dissecting the contribution of main-sequence (MS) and starburst (SB) galaxies. For each galaxy population, we convolved the observed galaxy stellar mass (M⋆_{\star}) function with a grid of M⋆_{\star}-independent Eddington ratio (λEDDλ_{\rm EDD}) distributions, normalised via empirical black hole accretion rate (BHAR) to star formation rate (SFR) relations. Our simple approach yields an excellent agreement with the observed XLF since z∼\sim3. We find that the redshift evolution of the observed XLF can only be reproduced through an intrinsic flattening of the λEDDλ_{\rm EDD} distribution, and with a positive shift of the break λ∗λ^{*}, consistent with an anti-hierarchical behavior. The AGN accretion history is predominantly made by massive (1010<^{10}<M⋆<_{\star}<1011^{11} M⊙_{\odot}) MS galaxies, while SB-driven BH accretion, possibly associated with galaxy mergers, becomes dominant only in bright quasars, at log⁡\log(LX_{\rm X}/erg s−1^{-1})>>44.36 + 1.28⋅\cdot(1+z). We infer that the probability of finding highly-accreting (λEDD>λ_{\rm EDD}> 10%) AGN significantly increases with redshift, from 0.4% (3.0%) at z=0.5 to 6.5% (15.3%) at z=3 for MS (SB) galaxies, implying a longer AGN duty cycle in the early Universe. Our results strongly favor a M⋆_{\star}-dependent ratio between BHAR and SFR, as BHAR/SFR ∝\propto M⋆0.73[+0.22,−0.29]_{\star}^{0.73[+0.22,-0.29]}, supporting a non-linear BH buildup relative to the host. Finally, this framework opens potential questions on super-Eddington BH accretion and different λEDDλ_{\rm EDD} prescriptions for understanding the cosmic BH mass assembly.

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