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Entropy of 4D extremal black holes

We derive the Bekenstein-Hawking entropy formula for four-dimensional Reissner-Nordstr\"om extremal black holes in type II string theory. The derivation is performed in two separate (T-dual) weak coupling pictures. One uses a type IIB bound state problem of D5- and D1-branes, while the other us...

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Detalles Bibliográficos
Autores principales: Johnson, Clifford V., Khuri, Ramzi R., Myers, Robert C.
Lenguaje:eng
Publicado: 1996
Materias:
Acceso en línea:https://dx.doi.org/10.1016/0370-2693(96)00383-8
http://cds.cern.ch/record/298470
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author Johnson, Clifford V.
Khuri, Ramzi R.
Myers, Robert C.
author_facet Johnson, Clifford V.
Khuri, Ramzi R.
Myers, Robert C.
author_sort Johnson, Clifford V.
collection CERN
description We derive the Bekenstein-Hawking entropy formula for four-dimensional Reissner-Nordstr\"om extremal black holes in type II string theory. The derivation is performed in two separate (T-dual) weak coupling pictures. One uses a type IIB bound state problem of D5- and D1-branes, while the other uses a bound state problem of D0- and D4-branes with macroscopic fundamental type IIA strings. In both cases the D-brane systems are also bound to a Kaluza-Klein monopole, which then yields the four-dimensional black hole at strong coupling.
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institution Organización Europea para la Investigación Nuclear
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spelling cern-2984702023-03-14T18:08:59Zdoi:10.1016/0370-2693(96)00383-8http://cds.cern.ch/record/298470engJohnson, Clifford V.Khuri, Ramzi R.Myers, Robert C.Entropy of 4D extremal black holesParticle Physics - TheoryWe derive the Bekenstein-Hawking entropy formula for four-dimensional Reissner-Nordstr\"om extremal black holes in type II string theory. The derivation is performed in two separate (T-dual) weak coupling pictures. One uses a type IIB bound state problem of D5- and D1-branes, while the other uses a bound state problem of D0- and D4-branes with macroscopic fundamental type IIA strings. In both cases the D-brane systems are also bound to a Kaluza-Klein monopole, which then yields the four-dimensional black hole at strong coupling.We derive the Bekenstein-Hawking entropy formula for four-dimensional Reissner-Nordstr\"om extremal black holes in type II string theory. The derivation is performed in two separate (T-dual) weak coupling pictures. One uses a type IIB bound state problem of D5- and D1-branes, while the other uses a bound state problem of D0- and D4-branes with macroscopic fundamental type IIA strings. In both cases, the D-brane systems are also bound to a Kaluza-Klein monopole, which then yields the four-dimensional black hole at strong coupling.We derive the Bekenstein-Hawking entropy formula for four-dimensional Reissner-Nordström extremal black holes in type II string theory. The derivation is performed in two separate (T-dual) weak coupling pictures. One uses a type IIB bound state problem of D5- and D1-branes, while the other uses a bound state problem of D0- and D4-branes with macroscopic fundamental type IIA strings. In both cases, the D-brane systems are also bound to a Kaluza-Klein monopole, which then yields the four-dimensional black hole at strong coupling.hep-th/9603061CERN-TH-96-62NSF-ITP-96-14MCGILL-96-09CERN-TH-96-062MCGILL-96-09NSF-ITP-96-14oai:cds.cern.ch:2984701996-03-10
spellingShingle Particle Physics - Theory
Johnson, Clifford V.
Khuri, Ramzi R.
Myers, Robert C.
Entropy of 4D extremal black holes
title Entropy of 4D extremal black holes
title_full Entropy of 4D extremal black holes
title_fullStr Entropy of 4D extremal black holes
title_full_unstemmed Entropy of 4D extremal black holes
title_short Entropy of 4D extremal black holes
title_sort entropy of 4d extremal black holes
topic Particle Physics - Theory
url https://dx.doi.org/10.1016/0370-2693(96)00383-8
http://cds.cern.ch/record/298470
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