Cargando…
New black hole, string and membrane solutions of the four-dimensional heterotic string
We present solutions of the low-energy four-dimensional heterotic string corresponding to $p$-branes with $p=0,1,2$, which are characterized by a mass per unit $p$-volume, ${\cal M}_{p+1}$, and topological ``magnetic'' charge, $g_{p+1}$. In the extremal limit, $\sqrt{2} \kappa {\cal M}_{p+...
Autores principales: | , , , |
---|---|
Lenguaje: | eng |
Publicado: |
1994
|
Materias: | |
Acceso en línea: | https://dx.doi.org/10.1016/0550-3213(94)90244-5 http://cds.cern.ch/record/255456 |
_version_ | 1780885765793775616 |
---|---|
author | Duff, M.J. Khuri, Ramzi R. Minasian, Ruben Rahmfeld, Joachim |
author_facet | Duff, M.J. Khuri, Ramzi R. Minasian, Ruben Rahmfeld, Joachim |
author_sort | Duff, M.J. |
collection | CERN |
description | We present solutions of the low-energy four-dimensional heterotic string corresponding to $p$-branes with $p=0,1,2$, which are characterized by a mass per unit $p$-volume, ${\cal M}_{p+1}$, and topological ``magnetic'' charge, $g_{p+1}$. In the extremal limit, $\sqrt{2} \kappa {\cal M}_{p+1} = g_{p+1}$, they reduce to the recently discovered non-singular supersymmetric monopole, string and domain wall solutions. A novel feature is that the solutions involve both the dilaton and the modulus fields. In particular, 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 $\alpha=1$. This means that electric/magnetic duality in $D=4$ may be seen as a consequence of string/fivebrane duality in $D=10$. |
id | cern-255456 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 1994 |
record_format | invenio |
spelling | cern-2554562020-07-23T02:48:32Zdoi:10.1016/0550-3213(94)90244-5http://cds.cern.ch/record/255456engDuff, M.J.Khuri, Ramzi R.Minasian, RubenRahmfeld, JoachimNew black hole, string and membrane solutions of the four-dimensional heterotic stringGeneral Theoretical PhysicsParticle Physics - TheoryWe present solutions of the low-energy four-dimensional heterotic string corresponding to $p$-branes with $p=0,1,2$, which are characterized by a mass per unit $p$-volume, ${\cal M}_{p+1}$, and topological ``magnetic'' charge, $g_{p+1}$. In the extremal limit, $\sqrt{2} \kappa {\cal M}_{p+1} = g_{p+1}$, they reduce to the recently discovered non-singular supersymmetric monopole, string and domain wall solutions. A novel feature is that the solutions involve both the dilaton and the modulus fields. In particular, 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 $\alpha=1$. This means that electric/magnetic duality in $D=4$ may be seen as a consequence of string/fivebrane duality in $D=10$.We present solutions of the low-energy four-dimensional heterotic string corresponding to $p$-branes with $p=0,1,2$, which are characterized by a mass per unit $p$-volume, ${\cal M}_{p+1}$, and topological ``magnetic'' charge, $g_{p+1}$. In the extremal limit, $\sqrt{2} \kappa {\cal M}_{p+1} = g_{p+1}$, they reduce to the recently discovered non-singular supersymmetric monopole, string and domain wall solutions. A novel feature is that the solutions involve both the dilaton and the modulus fields. In particular, 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 $\alpha=1$. This means that electric/magnetic duality in $D=4$ may be seen as a consequence of string/fivebrane duality in $D=10$.We present solutions of the low-energy four-dimensional heterotic string corresponding to p -branes with p =0, 1, 2, which are characterized by a mass per unit p -volume, M p+1 , and topological “magnetic” charge, g p +1 . In the extremal limit, √2ϰ M p+1 =g p+1 , they reduce to the recently discovered nonsingular supersymmetric monopole, string and domain wall solutions. A novel feature is that the solutions involve both the dilaton and the modulus fields. In particular, the effective scalar coupling to the Maxwell field, e − αφ F μν F μν , gives rise to a new string black hole with α =√3, in contrast to the pure dilaton black hole solution which has α =1. This means that electric/magnetic duality in D =4 may be seen as a consequence of string/fivebrane duality in D =10.hep-th/9311120CTP-TAMU-49-93CERN-TH-7088-93CERN-TH-7088-93CTP-TAMU-93-49oai:cds.cern.ch:2554561994 |
spellingShingle | General Theoretical Physics Particle Physics - Theory Duff, M.J. Khuri, Ramzi R. Minasian, Ruben Rahmfeld, Joachim New black hole, string and membrane solutions of the four-dimensional heterotic string |
title | New black hole, string and membrane solutions of the four-dimensional heterotic string |
title_full | New black hole, string and membrane solutions of the four-dimensional heterotic string |
title_fullStr | New black hole, string and membrane solutions of the four-dimensional heterotic string |
title_full_unstemmed | New black hole, string and membrane solutions of the four-dimensional heterotic string |
title_short | New black hole, string and membrane solutions of the four-dimensional heterotic string |
title_sort | new black hole, string and membrane solutions of the four-dimensional heterotic string |
topic | General Theoretical Physics Particle Physics - Theory |
url | https://dx.doi.org/10.1016/0550-3213(94)90244-5 http://cds.cern.ch/record/255456 |
work_keys_str_mv | AT duffmj newblackholestringandmembranesolutionsofthefourdimensionalheteroticstring AT khuriramzir newblackholestringandmembranesolutionsofthefourdimensionalheteroticstring AT minasianruben newblackholestringandmembranesolutionsofthefourdimensionalheteroticstring AT rahmfeldjoachim newblackholestringandmembranesolutionsofthefourdimensionalheteroticstring |