Journal
ASTROPHYSICAL JOURNAL
Volume 735, Issue 1, Pages -Publisher
IOP PUBLISHING LTD
DOI: 10.1088/0004-637X/735/1/9
Keywords
accretion, accretion disks; black hole physics; Galaxy: center; magnetohydrodynamics (MHD); radiative transfer
Categories
Funding
- National Science Foundation [AST 07-09246]
- NASA [NNX10AD03G]
- University Scholar appointment and a Richard and Margaret Romano Professorial Scholarship
- National Science Foundation through TeraGrid resources provided by TACC [TG-AST090007]
- NASA [NNX10AD03G, 135909] Funding Source: Federal RePORTER
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Electron-positron pairs may be produced near accreting black holes by a variety of physical processes, and the resulting pair plasma may be accelerated and collimated into a relativistic jet. Here, we use a self-consistent dynamical and radiative model to investigate pair production by gamma gamma collisions in weakly radiative accretion flows around a black hole of mass M and accretion rate (M) over dot. Our flow model is drawn from general relativistic magnetohydrodynamic simulations, and our radiation field is computed by a Monte Carlo transport scheme assuming the electron distribution function is thermal. We argue that the pair production rate scales as r(-6) M-1 (M) over dot(6). We confirm this numerically and calibrate the scaling relation. This relation is self-consistent in a wedge in M, (M) over dot parameter space. If (M) over dot is too low the implied pair density over the poles of the black hole is below the Goldreich-Julian density and gamma gamma pair production is relatively unimportant; if (M) over dot is too high the models are radiatively efficient. We also argue that for a power-law spectrum the pair production rate should scale with the observables LX = X-ray luminosity and M as L-X(2) M-4. We confirm this numerically and argue that this relation likely holds even for radiatively efficient flows. The pair production rates are sensitive to black hole spin and to the ion-electron temperature ratio which are fixed in this exploratory calculation. We finish with a brief discussion of the implications for Sgr A* and M87.
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