4.7 Article

Three-dimensional simulations of supercritical black hole accretion discs - luminosities, photon trapping and variability

Journal

MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY
Volume 456, Issue 4, Pages 3929-3947

Publisher

OXFORD UNIV PRESS
DOI: 10.1093/mnras/stv2941

Keywords

accretion, accretion discs; black hole physics; relativistic processes; methods: numerical

Funding

  1. NASA through Einstein Postdoctotral Fellowship by the Chandra X-ray Center [PF4-150126]
  2. NASA [NAS8-03060, TCAN NNX14AB47G]
  3. NSF [AST1312651]
  4. NSF via XSEDE resources [TG-AST080026N]
  5. Division Of Astronomical Sciences
  6. Direct For Mathematical & Physical Scien [1312651] Funding Source: National Science Foundation

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We present a set of four three-dimensional, general relativistic, radiation magnetohydrodynamical simulations of black hole accretion at supercritical mass accretion rates, (M) over dot > (M) over dot(Edd). We use these simulations to study how disc properties are modified when we vary the black hole mass, the black hole spin, or the mass accretion rate. In the case of a non-rotating black hole, we find that the total efficiency is of the order of 3 per cent (M) over dotc(2), approximately a factor of 2 less than the efficiency of a standard thin accretion disc. The radiation flux in the funnel along the axis is highly super-Eddington, but only a small fraction of the energy released by accretion escapes in this region. The bulk of the 3 per cent (M) over dotc(2) of energy emerges farther out in the disc, either in the form of photospheric emission or as a wind. In the case of a black hole with a spin parameter of 0.7, we find a larger efficiency of about 8 per cent (M) over dotc(2). By comparing the relative importance of advective and diffusive radiation transport, we show that photon trapping is effective near the equatorial plane. However, near the disc surface, vertical transport of radiation by diffusion dominates. We compare the properties of our fiducial three-dimensional run with those of an equivalent two-dimensional axisymmetric model with a mean-field dynamo. The latter simulation runs nearly 100 times faster than the three-dimensional simulation, and gives very similar results for time-averaged properties of the accretion flow, but does not reproduce the time-variability.

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