4.7 Article

Radiative, two-temperature simulations of low-luminosity black hole accretion flows in general relativity

Journal

MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY
Volume 466, Issue 1, Pages 705-725

Publisher

OXFORD UNIV PRESS
DOI: 10.1093/mnras/stw3116

Keywords

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

Funding

  1. NASA [PF4-150126, NAS8-03060, TCAN NNX 14AB7G]
  2. NSF [AST 1312651]
  3. NSF via XSEDE [TG-AST080026N]
  4. NASA Advanced Supercomputing (NAS) Division at Ames Research Center
  5. International Space Science Institute
  6. Polish NCN [UMO2013/08/A/ST9/00795]
  7. Foundation for Polish Science
  8. Chandra X-ray Center
  9. Division Of Astronomical Sciences
  10. Direct For Mathematical & Physical Scien [1312651] Funding Source: National Science Foundation

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We present a numerical method that evolves a two-temperature, magnetized, radiative, accretion flow around a black hole, within the framework of general relativistic radiation magnetohydrodynamics. As implemented in the code KORAL, the gas consists of two sub-components ions and electrons - which share the same dynamics but experience independent, relativistically consistent, thermodynamical evolution. The electrons and ions are heated independently according to a prescription from the literature for magnetohydrodynamical turbulent dissipation. Energy exchange between the particle species via Coulomb collisions is included. In addition, electrons gain and lose energy and momentum by absorbing and emitting synchrotron and bremsstrahlung radiation and through Compton scattering. All evolution equations are handled within a fully covariant framework in the relativistic fixed-metric space-time of the black hole. Numerical results are presented for five models of low-luminosity black hole accretion. In the case of a model with a mass accretion rate M similar to 4 x 10(-8) M-Edd, we find that radiation has a negligible effect on either the dynamics or the thermodynamics of the accreting gas. In contrast, a model with a larger M similar to 4 x 10(-4) M-Edd behaves very differently. The accreting gas is much cooler and the flow is geometrically less thick, though it is not quite a thin accretion disc.

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