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Black hole solutions in string theory

We present two-parameter solutions of the low-energy four-dimensional heterotic string which in the extremal limit reduce to supersymmetric monopole, string and domain wall solutions. The effective scalar coupling to the Maxwell field, e^{-\alpha \phi} F_{\mu\nu} F^{\mu\nu}, gives rise to a new stri...

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Detalles Bibliográficos
Autor principal: Khuri, Ramzi R.
Lenguaje:eng
Publicado: 1994
Materias:
Acceso en línea:http://cds.cern.ch/record/273955
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author Khuri, Ramzi R.
author_facet Khuri, Ramzi R.
author_sort Khuri, Ramzi R.
collection CERN
description We present two-parameter solutions of the low-energy four-dimensional heterotic string which in the extremal limit reduce to supersymmetric monopole, string and domain wall solutions. The effective scalar coupling to the Maxwell field, e^{-\alpha \phi} F_{\mu\nu} F^{\mu\nu}, gives rise to a new string black hole with \alpha = \sqrt{3}, in contrast to the pure dilaton black hole solution which has \alpha=1. Implications of string/fivebrane duality in D=10 to four-dimensional dualities are discussed.
id cern-273955
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1994
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spelling cern-2739552020-07-23T02:49:19Zhttp://cds.cern.ch/record/273955engKhuri, Ramzi R.Black hole solutions in string theoryGeneral Theoretical PhysicsParticle Physics - TheoryWe present two-parameter solutions of the low-energy four-dimensional heterotic string which in the extremal limit reduce to supersymmetric monopole, string and domain wall solutions. The effective scalar coupling to the Maxwell field, e^{-\alpha \phi} F_{\mu\nu} F^{\mu\nu}, gives rise to a new string black hole with \alpha = \sqrt{3}, in contrast to the pure dilaton black hole solution which has \alpha=1. Implications of string/fivebrane duality in D=10 to four-dimensional dualities are discussed.We present two-parameter solutions of the low-energy four-dimensional heterotic string which in the extremal limit reduce to supersymmetric monopole, string and domain wall solutions. The effective scalar coupling to the Maxwell field, $e~{-\alpha \phi} F_{\mu\nu} F~{\mu\nu}$, gives rise to a new string black hole with $\alpha = \sqrt{3}$, in contrast to the pure dilaton black hole solution which has $\alpha=1$. Implications of string/fivebrane duality in $D=10$ to four-dimensional dualities are discussed.hep-th/9412150CERN-TH-7467-94MCGILL-94-51CERN-TH-7467-94oai:cds.cern.ch:2739551994
spellingShingle General Theoretical Physics
Particle Physics - Theory
Khuri, Ramzi R.
Black hole solutions in string theory
title Black hole solutions in string theory
title_full Black hole solutions in string theory
title_fullStr Black hole solutions in string theory
title_full_unstemmed Black hole solutions in string theory
title_short Black hole solutions in string theory
title_sort black hole solutions in string theory
topic General Theoretical Physics
Particle Physics - Theory
url http://cds.cern.ch/record/273955
work_keys_str_mv AT khuriramzir blackholesolutionsinstringtheory