Journal
MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY
Volume 453, Issue 3, Pages 3213-3221Publisher
OXFORD UNIV PRESS
DOI: 10.1093/mnras/stv1802
Keywords
accretion, accretion discs; black hole physics; relativistic processes; galaxies: jets; X-rays: individual: Sw J1644+57; X-rays: individual: SS433; X-rays: ULX
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Funding
- NASA through Einstein Postdoctotral Fellowship - Chandra X-ray Center under NASA [PF4-150126, NAS8-03060]
- NSF [AST1312651]
- NASA [TCAN NNX14AB47G]
- NSF via XSEDE [TG-AST080026N]
- Division Of Astronomical Sciences
- Direct For Mathematical & Physical Scien [1312651] Funding Source: National Science Foundation
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We describe a set of simulations of supercritical accretion on to a non-rotating supermassive black hole (BH). The accretion flow takes the form of a geometrically thick disc with twin low-density funnels around the rotation axis. For accretion rates greater than or similar to 10. M-Edd, there is sufficient gas in the funnel to make this region optically thick. Radiation from the disc first flows into the funnel, after which it accelerates the optically thick funnel gas along the axis. The resulting jet is baryon loaded and has a terminal density-weighted velocity approximate to 0.3c. Much of the radiative luminosity is converted into kinetic energy by the time the escaping gas becomes optically thin. These jets are not powered by BHrotation or magnetic driving, but purely by radiation. Their characteristic beaming angle is similar to 0.2 rad. For an observer viewing down the axis, the isotropic equivalent luminosity of total energy is as much as 10(48) erg s(-1) for a 10(7) M-circle dot BH accreting at 10(3) Eddington. Therefore, energetically, the simulated jets are consistent with observations of the most powerful tidal disruption events, e.g. Swift J1644. The jet velocity is, however, too low to match the Lorentz factor gamma > 2 inferred in J1644. There is no such conflict in the case of other tidal disruption events. Since favourably oriented observers see isotropic equivalent luminosities that are highly super-Eddington, the simulated models can explain observations of ultraluminous X-ray sources, at least in terms of luminosity and energetics, without requiring intermediate-mass BHs.
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