Abstract

This review covers the main aspects of black hole accretion disk theory. We begin with the view that one of the main goals of the theory is to better understand the nature of black holes themselves. In this light we discuss how accretion disks might reveal some of the unique signatures of strong gravity: the event horizon, the innermost stable circular orbit, and the ergosphere. We then review, from a first-principles perspective, the physical processes at play in accretion disks. This leads us to the four primary accretion disk models that we review: Polish doughnuts (thick disks), Shakura-Sunyaev (thin) disks, slim disks, and advection-dominated accretion flows (ADAFs). After presenting the models we discuss issues of stability, oscillations, and jets. Following our review of the analytic work, we take a parallel approach in reviewing numerical studies of black hole accretion disks. We finish with a few select applications that highlight particular astrophysical applications: measurements of black hole mass and spin, black hole vs. neutron star accretion disks, black hole accretion disk spectral states, and quasi-periodic oscillations (QPOs).

Highlights

  • Because of its firm connection to black holes themselves, black hole accretion disk theory belongs to the realm of fundamental physics

  • 2 Three Destinations in Kerr’s Strong Gravity we briefly describe the three destinations within Kerr’s strong gravity that are most relevant to black hole accretion disk theory: 1. Event Horizon: That radius inside of which escape from the black hole is not possible; 2

  • The right-hand side of the energy equation (93) represents advective cooling. This is assumed to vanish in the Shakura–Sunyaev model, though we will see that it plays a critical role in slim disks (Section 6) and advection-dominated accretion flows (ADAFs) (Section 7)

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Summary

Introduction

Because of its firm connection to black holes themselves, black hole accretion disk theory belongs to the realm of fundamental physics. In our theory-minded Living Review we do not give detailed descriptions of their observational properties Instead, we stress their importance by starting our road map from the two classes of observed black holes: Destination 1: Quasars and other similar supermassive objects, which are collectively called “active galactic nuclei” (or AGN), having masses in the range 106 M⊙ < M < 109 M⊙. There is an important overlap region where various analytic and numerical methods are applicable and can be used to independently validate results Because of these close connections between analytic and numerical work, we have dedicated Section 11 to the discussion and review of direct numerical simulation of black hole accretion disks. We follow the common convention where Greek (Latin) indices are used for four-(three-)dimensional tensor quantities

Three Destinations in Kerr’s Strong Gravity
The event horizon
Detecting the event horizon
The ergosphere
ISCO: the orbit of marginal stability
The Paczynski–Wiita potential
Summary: characteristic radii and frequencies
Matter Description
The fluid part
Perfect fluid
The stress part
The alpha viscosity prescription
The Maxwell part
The radiation part
Bremsstrahlung
Synchrotron
Comptonization
Polish doughnuts
Magnetized Tori
Thin Disks
Equations in the Kerr geometry
The eigenvalue problem
Solutions
Slim Disks
Stability
Hydrodynamic stability
Runaway instability
Thermal and viscous instability
Oscillations
Dynamical oscillations of thick disks
Diskoseismology: oscillations of thin disks
10 Relativistic Jets
11.1.1 Computational fluid dynamics codes
11.2 Matter description in simulations
11.2.4 Evolving GRMHD
11.5 ADAFs in simulations
11.6 Oscillations in simulations
11.7 Jets in simulations
11.8 Highly magnetized accretion in simulations
12.1 Measurements of black-hole mass and spin
12.3 Black-hole accretion disk spectral states
12.5 The case of Sgr A*
13 Concluding Remarks
14 Acknowledgements
Full Text
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