The brief era of direct collapse black hole formation
arXiv:1402.5675 · doi:10.1093/mnras/stu351
Abstract
It has been proposed that the first, intermediate-mass () black holes might form through direct collapse of unpolluted gas in atomic-cooling halos exposed to a strong Lyman-Werner (LW) or near-infrared (NIR) radiation. As these systems are expected to be Compton-thick, photons above 13.6 eV are largely absorbed and re-processed into lower energy bands. It follows that direct collapse black holes (DCBHs) are very bright in the LW/NIR bands, typically outshining small high-redshift galaxies by more than 10 times. Once the first DCBHs form, they then trigger a runaway process of further DCBH formation, producing a sudden rise in their cosmic mass density. The universe enters the "DCBH era" at when a large fraction of atomic-cooling halos are experiencing DCBH formation. By combining the clustering properties of the radiation sources with Monte Carlo simulations we show that in this scenario the DCBH mass density rises from ~ Mpc at to the peak value Mpc at in our fiducial model. However, the abundance of \textit{active} (accreting) DCBHs drops after , as gas in the potential formation sites (unpolluted halos with virial temperature slightly above ~K) is photoevaporated. This effect almost completely suppresses DCBH formation after . The DCBH formation era lasts only Myr, but it might crucially provide the seeds of the supermassive black holes (SMBHs) powering quasars.
26 pages, 4 figures, 2 tables. Accepted for publication in MNRAS
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