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Supermassive black hole formation by direct collapse: keeping protogalactic gas H<sub>2</sub>free in dark matter haloes with virial temperatures<i>T</i><sub>vir</sub>&gt;<i>rsim</i> <i>10<sup>4</sup></i>K

Cien ShangDepartment of Physics, Columbia University, 538 West 120th Street, New York, NY 10027, USAGreg L. BryanDepartment of Astronomy, Columbia University, 550 West 120th Street, New York, NY 10027, USAZoltán HaimanDepartment of Astronomy, Columbia University, 550 West 120th Street, New York, NY 10027, USA
2009en
ABI

Аннотация

In the absence of H 2 molecules, the primordial gas in early dark matter haloes with virial temperatures just above T vir 10 4 K cools by collisional excitation of atomic H. Although it cools efficiently, this gas remains relatively hot, at a temperature near T 8000 K, and consequently might be able to avoid fragmentation and collapse directly into a supermassive black hole. In order for H 2 formation and cooling to be strongly suppressed, the gas must be irradiated by a sufficiently intense ultraviolet (UV) flux. We performed a suite of threedimensional hydrodynamical adaptive mesh refinement (AMR) simulations of gas collapse in three different protogalactic haloes with T vir 10 4 K, irradiated by a UV flux with various intensities and spectra. We determined the critical specific intensity, J crit 21 , required to suppress H 2 cooling in each of the three haloes. For a hard spectrum representative of metal-free stars, we find (in units of 10 -21 erg s -1 Hz -1 sr -1 cm -2 ) 10 4 < J crit 21 < 10 5 , while for a softer spectrum, which is characteristic of a normal stellar population, and for which H -dissociation is important, we find 30 < J crit 21 < 300. These values are a factor of 3-10 lower than previous estimates. We attribute the difference to the higher, more accurate H 2 collisional dissociation rate we adopted. The reduction in J crit 21 exponentially increases the number of rare haloes exposed to supercritical radiation. When H 2 cooling is suppressed, gas collapse starts with a delay, but it ultimately proceeds more rapidly. The infall velocity is near the increased sound speed, and an object as massive as M 10 5 M may form at the centre of these haloes, compared to the M 10 2 M stars forming when H 2 cooling is efficient.

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