Black Hole Entropy  

In General > s.a. black hole thermodynamics; gravitational phenomenology [spacetime measurement]; specific types of black holes.
* Idea: Black hole entropy was introduced in a formal way; Several interpretations of it have been proposed, some of which are variations on Bekenstein's original idea that it corresponds to the log of "distinct quantum internal states" of the black hole, S = kB ln W, but in general it is not clear what this W means physically; Classically, one has to use S = to avoid inconsistencies with the second law, but quantum mechanically there is black hole radiation and all is ok.
* Schwarzschild: A Schwarzschild black hole of classical surface area AH has entropy (in any dimension)

SB = (kBc3/G) AH .

* Reissner-Nordström: An extremal black hole has S = 0 but A 0.
* Remark: With matter fields, in general S A/4; It is possible to form black holes without a global increase in entropy.
* Orders of magnitude: Compare SSun = 1058 with Ssolar mass bh = 1077.
@ Reviews: Mitra ht/96; Frolov & Fursaev CQG(98)ht; Majumdar gq/98-in, ht/01-in; Mukohyama gq/99-in; Damour ht/04-in; Jacobson et al ht/05-in [trialogue on interpretation]; Soloviev gq/05-in.
@ General references: Wald PRD(79); Gould PRD(87); Martinez & York PRD(89); Hiscock PRD(89); Frolov & Novikov PRD(93)gq; Wald PRD(93)gq [Noether charge]; Dowker CQG(94); Teitelboim ht/94 [and dimensional continuation]; Frolov ht/94-in, ht/95-in; Jacobson et al PRD(94)gq/93; Brown & York gq/94-in [path integral]; Martinez PRD(95)gq/94 [microcanonical]; Brown PRD(95)gq [from Hamiltonian]; Pretorius et al PRD(98)gq/97 [operational]; Kay ht/98; Mäkelä & Repo gq/98; Lue & Weinberg GRG(00)gq [and monopoles]; Major & Setter CQG(01) [universality]; Medved gq/04 [re interpretation]; Sorkin SHPMP(05)ht-in [point of view]; Cadoni MPLA(06)ht/05; Jacobson et al IJTP(05) [views]; Carlip gq/07-in, GRG(07)-a0705-GRF [the problem of universality].
@ Properties: Iyer & Wald PRD(94)gq, PRD(95)gq; Lau gq/94; Bekenstein gq/94-in; Solodukhin PRD(96) [approaches agree]; Corichi & Sudarsky MPLA(02)gq/00 [and area]; Åman et al GRG(03)gq [and state space metric].

From Black Hole Microstates > s.a. 2D gravity; quantum black holes.
@ Fluctuations: Gerlach PRD(76); York PRD(83), in(84); Pavón & Rubí PRD(88); Frolov PRL(95); Sorkin & Sudarsky CQG(99)gq; Gour & Medved CQG(03)gq; Requardt a0708.
@ Spacetime microstructure: Scardigli CQG(97)gq [foam]; Padmanabhan PRL(98)ht; Garattini Ent(00)gq [foam, Schwarzschild-de Sitter], IJMPD(02)gq/00; Bergamin & Grumiller IJMPD(06)gq-GRF.
@ Strings, M-theory: Horowitz & Strominger PRL(96) [near extremal]; Strominger & Vafa PLB(96); Horowitz & Marolf PRD(97)ht/96; Maldacena et al JHEP(97)ht, Horowitz & Roberts PRL(07) [extremal, in M-theory]; Lowe PRL(98); Dabholkar IJMPD(06).
@ Horizon cft: Carlip gq/95, gq/96-in, PRD(97)gq/96 [3D], NPPS(97)gq, PRL(99)ht/98, CQG(99)gq, gq/99-in; Park NPB(02)ht/01 [deformations]; Carlip CQG(05)ht/04 [stretched horizon], gq/05-in, IJTP(07)gq/06-in [horizon constraints and symmetry algebra].
@ Horizon microstates: Sfetsos & Skenderis NPB(98)ht/97; Brown PRD(98); Epp & Mann MPLA(98)gq, Epp gq/98/PRD [tetrad approach]; Cvetic & Larsen PRL(99) [rotating]; Soloviev PRD(00)ht/99; Dou & Sorkin FP(03)gq, Rideout & Zohren gq/06-in [causal links]; Das & Shankaranarayanan gq/07.
@ Loop quantum gravity: Garay & Mena CQG(03), Ghosh & Mitra PLB(05)gq/04 [and Immirzi parameter]; Domagala & Lewandowski CQG(04)gq; Meissner CQG(04)gq; Swain IJMPD(05)gq-GRF; Mitra a0705-in [state counting]; Tamaki CQG(07)-a0707; Jacobson CQG(07)-a0708 [and renormalization]; Sahlmann PRD(07)-a0709.

Other Origin and Approaches > s.a. horizons.
* Ways of forming the black hole: S is the log of the number of quantum mechanically distinct ways that the black hole could have been made, or information lost in the creation of the black hole; This leads to an estimate of the quantum black hole level spacing.
* Entanglement entropy: Black hole entropy is semi-classical, in the sense that it comes from tracing out over internal degrees of freedom of quantum fields in a classical geometry, without even backreaction – related to the "brick wall model" idea; Appears to be proportional to A for fields in the ground state or in coherent/squeezed states, not in excited states.
@ Ways of forming the black hole: Zurek & Thorne PRL(85); & Bekenstein; & Hawking; Mukhanov FP(03); Hsu & Reeb a0706 [and monster states].
@ Entanglement entropy: Sorkin in(83); Bombelli et al PRD(86); Srednicki PRL(93); Jacobson gq/94 [and induced gravity]; Kabat NPB(95)ht [and 1-loop corrections]; Muller & Loustó PRD(95); Ahmadi et al ht/05-in [deviations from area law]; Ansari NPB(08)gq/06 [in lqg]; Emparan JHEP(06) [holographic derivation]; Das & Shankaranarayanan gq/06-in, Das et al a0705, a0708-in [power-law corrections in different states]; Brout a0802 [independence of number of species]; Das et al a0806-in [rev].
@ And brick wall: Mukohyama et al PRD(97)gq; Mukohyama gq/98-PhD, gq/99-in; Jing & Yan PRD(99)gq [Kerr]; Garattini MPLA(04) [and spacetime foam].
@ Other proposals: Yang MPLA(01) [topological invariants]; Badiali JPA(06)gq/05 [spacetime order]; Banerjee et al a0804 [covariant anomalies].

Corrections > s.a. 2D gravity; 3D black holes; 3D quantum gravity; black hole radiation; quantum black holes; specific types of black holes.
* Reasons: Can be due to thermal fluctuations around an equilibrium canonical ensemble, or quantum spacetime fluctuations within a microcanonical framework; Typically, higher-order gravity theories give corrections of the form AH R, R2, etc, while various approaches to effective quantum gravity corrections give terms of the form ln AH.
@ From partition function: Gibbons & Hawking PRD(77); York PRD(86).
@ Quantum / log corrections: Susskind & Uglum PRD(94) [canonical quantum gravity and string theory]; Mitra gq/95-in; Ghosh & Mitra PRD(97); Carlip CQG(00)gq [log, Cardy formula]; Kaul & Majumdar PRL(00); Das et al CQG(02)ht/01, ht/02-in; Gour PRD(02)gq [log]; Mukherji & Pal JHEP(02)ht [AdS-cft]; Chatterjee & Majumdar gq/03, PRL(04)gq/03 [log, non-rotating]; Akbar & Das CQG(04)ht/03 [Schwarzschild and Reissner-Nordström, thermal]; Bhaduri et al PRD(04)gq/03 [microcanonical]; Ghosh & Mitra PRD(05)gq/04; Hod CQG(04)ht [higher-order]; Medved CQG(03) [2D], CQG(05)gq/04, CQG(05)gq/04; Medved & Vagenas PRD(04)ht [using gup]; Zhao et al MPLA(07)gq/06; Shankaranarayanan MPLA-a0805.
@ Renormalized: Odintsov & Yoon IJMPA(96)gq/95; Larsen & Wilczek NPB(96).
@ Higher-derivative gravity: Correa-Borbonet BJP(05)ht-in [Lovelock theory]; Kraus & Larsen JHEP(05)ht.
@ Related topics: Belgiorno & Liberati GRG(97)gq/96 [and Casimir effect]; Liberati NCB(97)gq/96 ["intrinsic" thermodynamics]; Strominger JHEP(98)ht/97 [AdS geometry]; Jacobson gq/99-in [partial horizon]; Wu IJMPD(00)gq [topology]; Dreyer et al CQG(01)gq [symmetries]; Carlip PRL(02)gq [conformal symmetry]; More CQG(05)gq/04 [higher-order corrections]; > s.a. entropy.

Other Related Topics > see fine structure constant [variation].


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