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The aftermath of the first stars: massive black holes
Author(s) -
Johnson Jarrett L.,
Bromm Volker
Publication year - 2007
Publication title -
monthly notices of the royal astronomical society
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 2.058
H-Index - 383
eISSN - 1365-2966
pISSN - 0035-8711
DOI - 10.1111/j.1365-2966.2006.11275.x
Subject(s) - physics , astrophysics , supermassive black hole , population , redshift , star formation , astronomy , stars , accretion (finance) , quasar , reionization , galaxy , demography , sociology
We investigate the evolution of the primordial gas surrounding the first massive black holes formed by the collapse of Population III stars at redshifts z ≳ 20 . Carrying out three‐dimensional hydrodynamical simulations using gadget , we study the dynamical, thermal and chemical evolution of the first relic H  ii regions. We also carry out simulations of the mergers of relic H  ii regions with neighbouring neutral minihaloes, which contain high‐density primordial gas that could accrete on to a Population III remnant black hole. We find that there may have been a significant time delay, of the order of ∼10 8 yr, between black hole formation and the onset of efficient accretion. The build‐up of supermassive black holes, believed to power the z ≳ 6 quasars observed in the Sloan Digital Sky Survey, therefore faces a crucial early bottleneck. More massive seed black holes may thus be required, such as those formed by the direct collapse of a primordial gas cloud facilitated by atomic line cooling. The high optical depth to Lyman–Werner (LW) photons that results from the high fraction of H 2 molecules that form in relic H  ii regions, combined with the continued formation of H 2 inside the dynamically expanding relic H  ii region, leads to shielding of the molecules inside these regions at least until a critical background LW flux of ∼10 −24 erg s −1 cm −2 Hz −1 sr −1 is established. Furthermore, we find that a high fraction of deuterium hydride (HD) molecules, X HD ≳ 10 −7 , is formed, potentially enabling the formation of Population II.5 stars, with masses of the order of ∼10 M ⊙ , during later stages of structure formation when the relic H  ii region gas is assembled into a sufficiently deep potential well to gravitationally confine the gas again.

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