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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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Lenguaje: | eng |
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1994
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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 |
record_format | invenio |
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 |