1998
DOI: 10.1016/s0370-2693(98)00236-6
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Entropy of three-dimensional black holes in string theory

Abstract: It is observed that the three-dimensional BTZ black hole is a supersymmetric solution of the low-energy field equations of heterotic string theory compactified on an Einstein space. The solution involves a non-zero dilaton and NS-NS H-field. The entropy of the extreme black hole can then be computed using string theory and the asymptotic properties of anti-de Sitter space, without recourse to a D-brane analysis. This provides an explicit example of a black hole whose entropy can be computed using fundamental s… Show more

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Cited by 116 publications
(133 citation statements)
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“…As observed in [37] the degeneracy of states for a conformal field theory with this central charge gives rise to, under appropriate conditions, exactly the Bekenstein-Hawking entropy for the 2 + 1 black hole (see also [38]). An earlier statistical description of the 2 + 1 black hole entropy was given by Carlip [39] in terms of horizon degrees of freedom.…”
Section: Discussionmentioning
confidence: 65%
“…As observed in [37] the degeneracy of states for a conformal field theory with this central charge gives rise to, under appropriate conditions, exactly the Bekenstein-Hawking entropy for the 2 + 1 black hole (see also [38]). An earlier statistical description of the 2 + 1 black hole entropy was given by Carlip [39] in terms of horizon degrees of freedom.…”
Section: Discussionmentioning
confidence: 65%
“…Notably, such a calculation has been considered for a rotating BTZ black hole [39,40]. Although it would be interesting to compare these results with our derivations, this seems impratical given the complexity of their expressions and the lack of compatibilty with the charged BTZ scenario.…”
Section: Resultsmentioning
confidence: 97%
“…As Strominger [7] and Birmingham, Sachs, and Sen [8] observed, these conformal weights and the central charges (27) then determine an entropy…”
Section: The Btz Black Holementioning
confidence: 87%