1998
DOI: 10.1046/j.1365-8711.1998.01530.x
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Super-Eddington accretion discs around Kerr black holes

Abstract: We calculate the structure of the accretion disc around a rapidly rotating black hole with a super‐Eddington accretion rate. The luminosity and height of the disc are reduced by the advection effect. In the case of large viscosity parameter, α>0.03, the accretion flow deviates strongly from thermodynamic equilibrium and overheats in the central region. With increasing accretion rate, the flow temperature steeply increases, reaches maximum, and then falls off. The maximum is achieved in the advection‐dominated … Show more

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Cited by 110 publications
(116 citation statements)
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“…For higher values of α their range of applicability is limited to lower luminosities (e.g., to 0.5L Edd for α = 0.1). Kerr-metric slim disks with low effective optical depth were discussed by Beloborodov (1998), who finds them to be significantly hotter than the optically thick ones. We have already started implementing a radiative transfer scheme valid for disks with small effective optical depths into the scheme introduced in this work.…”
Section: Discussionmentioning
confidence: 99%
“…For higher values of α their range of applicability is limited to lower luminosities (e.g., to 0.5L Edd for α = 0.1). Kerr-metric slim disks with low effective optical depth were discussed by Beloborodov (1998), who finds them to be significantly hotter than the optically thick ones. We have already started implementing a radiative transfer scheme valid for disks with small effective optical depths into the scheme introduced in this work.…”
Section: Discussionmentioning
confidence: 99%
“…1. (i) In the innermost regions (R < R ph,in ), the wind is essentially transparent (τ ≤ 1) and so the emission will appear as a distorted 'hot disc', peaking at a characteristic temperature, T in (modified by some colour temperature correction, spin and overheating; see Beloborodov 1998;Suleimanov et al 2002;Kawaguchi 2003).…”
Section: T H E S U P E R C R I T I C a L M O D E L O F Ac C R E T I O Nmentioning
confidence: 99%
“…Schematic representation of the supercritical model for bright (>3 × 10 39 erg s −1 ) ULXs (P07) where an optically thick wind is launched from the surface of a large scaleheight flow. This flow is driven from the disc from R sph (≈ṁ 0 R in ; Shakura & Sunyaev 1973) down to R ph,in within which the outflow is effectively transparent and the underlying disc emission can emerge (which may be further distorted by advection, spin and overheating; P07, Beloborodov 1998;Suleimanov et al 2002;Kawaguchi 2003). Variability due to obscuration/scattering can be introduced when the wind is inhomogeneous -expected on large scales via radial propagation of flux (Lyubarskii 1997) and seen on small scales in 2D MHD simulations (Takeuchi et al 2013(Takeuchi et al , 2014.…”
Section: T H E S U P E R C R I T I C a L M O D E L O F Ac C R E T I O Nmentioning
confidence: 99%
“…However, whether the Eddington limit should be applied or not needs to be further investigated, since the luminosity generated by accretion in excess of this limit might be carried away from the system via a strong wind, or transfered to a disc. SuperEddington accretion rates may be important for the formation of low-mass X-ray binaries and millisecond pulsars (Webbink & Kalogera 1997) and also for modeling X-ray emission from quasars due to accretion from a disc onto a fast rotating black hole (Beloborodov 1998). Imposing the limit diminishes the birth rate of type Ia supernovae (Livio 2000).…”
Section: Mass Transfer In Compact Binariesmentioning
confidence: 99%