Black-Hole Accretion Disks: Towards a New Paradigm
By S. Kato, J. Fukue, S. Mineshige. 2008
486 citations recorded by the source corpus.
View Paper: https://www.semanticscholar.org/paper/3d0bf85c3a4120e92672bdbdf932d617bf6f874e
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Citations in the corpus
- THE EVENT HORIZON OF SAGITTARIUS A* (2009, background): “…surface emission to remain undetected would require unphysically large radiative efficiencies, greater than 99.6%, as compared to the typical efficiencies in active galactic nuclei (AGNs) of 10% (Kato et al. 2008) and the meager efficiency implicated in Sgr A*, 0.01%–1% (Narayan & McClintock 2008).”
- Circularization of Tidally Disrupted Stars around Spinning Supermassive Black Holes (2015, background): “While the mass-to-energy conversion efficiency reaches ≈ 42% for an extreme Kerr black hole in a prograde rotation, it is only ≈ 4% for the retrograde case (Kato et al. 2008), suggesting a wide range of bolometric disk luminosities depending on the relative inclination of disk and SMBH spin.”
- GLOBAL STRUCTURE OF THREE DISTINCT ACCRETION FLOWS AND OUTFLOWS AROUND BLACK HOLES FROM TWO-DIMENSIONAL RADIATION-MAGNETOHYDRODYNAMIC SIMULATIONS (2011, background): “…inefficient accretion flow (RIAF) model, which are proposed as models for the accretion flow with higher (∼ LE) and lower luminosities, respectively (Shakura & Sunyaev 1973; Ichimaru 1977; Rees et al. 1982; Abramowicz et al. 1988; Narayan & Yi 1994, see Kato et al. 2008 for an extensive review).”
- Global Radiation-Magnetohydrodynamic Simulations of Black-Hole Accretion Flow and Outflow: Unified Model of Three States (2009, background): “For example, the disk viscosity, the most important key ingredient for the accretion disk theory, is prescribed by a phenomenological α-viscosity model, whereby the viscous torque is proportional to the pressure (Kato et al. 2008), although its physical basis is not clear.”
- Hot Accretion Flows Around Black Holes (2014, background): “…flow with viscous transport of angular momentum — is the celebrated thin disk model developed in the early 1970s (Shakura & Sunyaev 1973, Novikov & Thorne 1973, Lynden-Bell & Pringle 1974; see reviews by Pringle 1981, Frank et al. 2002, Kato et al. 2008, Abramowicz & Fragile 2013, Blaes 2013).”
- Neutrino-dominated accretion flows as the central engine of gamma-ray bursts (2017, background): “Here xms = 3 + Z2 − √ (3 − Z1)(3 + Z1 + 2Z2), where Z1 = 1 + (1 − a2∗)1/3[(1 + a∗)1/3 + (1 − a∗)1/3] and Z2 = √ 3a2∗ + Z 2 1 for 0 < a∗ < 1 (e.g., Bardeen et al. 1972; Kato et al. 2008; Zalamea & Beloborodov 2011; Liu et al. 2015c).”