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Constant magnetic field in closed string theory: an exactly solvable model

We consider a simple model describing a closed bosonic string in a constant magnetic field. Exact conformal invariance demands also the presence of a non-trivial metric and antisymmetric tensor (induced by magnetic field). The model is invariant under target space duality in a compact Kaluza-Klein d...

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Detalles Bibliográficos
Autores principales: Russo, J.G., Tseytlin, Arkady A.
Lenguaje:eng
Publicado: 1994
Materias:
Acceso en línea:https://dx.doi.org/10.1016/0550-3213(95)00091-6
http://cds.cern.ch/record/272126
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author Russo, J.G.
Tseytlin, Arkady A.
author_facet Russo, J.G.
Tseytlin, Arkady A.
author_sort Russo, J.G.
collection CERN
description We consider a simple model describing a closed bosonic string in a constant magnetic field. Exact conformal invariance demands also the presence of a non-trivial metric and antisymmetric tensor (induced by magnetic field). The model is invariant under target space duality in a compact Kaluza-Klein direction introduced to couple the magnetic field. Like open string theory in a constant gauge field, or closed string theory on a torus, this model can be straightforwardly quantized and solved with its spectrum of states and partition function explicitly computed. Above some critical value of the magnetic field an infinite number of states become tachyonic, suggesting a presence of phase transition. We also construct heterotic string generalisations of this bosonic model in which the constant magnetic field is embedded either in the Kaluza-Klein or internal gauge group sector.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1994
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spelling cern-2721262023-03-14T18:59:47Zdoi:10.1016/0550-3213(95)00091-6http://cds.cern.ch/record/272126engRusso, J.G.Tseytlin, Arkady A.Constant magnetic field in closed string theory: an exactly solvable modelParticle Physics - TheoryParticle Physics - TheoryWe consider a simple model describing a closed bosonic string in a constant magnetic field. Exact conformal invariance demands also the presence of a non-trivial metric and antisymmetric tensor (induced by magnetic field). The model is invariant under target space duality in a compact Kaluza-Klein direction introduced to couple the magnetic field. Like open string theory in a constant gauge field, or closed string theory on a torus, this model can be straightforwardly quantized and solved with its spectrum of states and partition function explicitly computed. Above some critical value of the magnetic field an infinite number of states become tachyonic, suggesting a presence of phase transition. We also construct heterotic string generalisations of this bosonic model in which the constant magnetic field is embedded either in the Kaluza-Klein or internal gauge group sector.We consider a simple model describing a closed bosonic string in a constant magnetic field. Exact conformal invariance demands also the presence of a non-trivial metric and antisymmetric tensor (induced by magnetic field). The model is invariant under target space duality in a compact Kaluza-Klein direction introduced to couple the magnetic field. Like open string theory in a constant gauge field, or closed string theory on a torus, this model can be straightforwardly quantized and solved with its spectrum of states and partition function explicitly computed. Above some critical value of the magnetic field an infinite number of states become tachyonic, suggesting a presence of phase transition. We also construct heterotic string generalisations of this bosonic model in which the constant magnetic field is embedded either in the Kaluza-Klein or internal gauge group sector.We consider a simple model describing a closed bosonic string in a constant magnetic field. Exact conformal invariance demands also the presence of a non-trivial metric and antisymmetric tensor (induced by magnetic field). The model is invariant under target space duality in a compact Kaluza-Klein direction introduced to couple the magnetic field. Like open string theory in a constant gauge field, or closed string theory on a torus, this model can be straightforwardly quantized and solved with its spectrum of states and partition function explicitly computed. Above some critical value of the magnetic field an infinite number of states become tachyonic, suggesting a presence of phase transition. We also construct heterotic string generalisations of this bosonic model in which the constant magnetic field is embedded either in the Kaluza-Klein or internal gauge group sector.We consider a simple model describing a closed bosonic string in a constant magnetic field. Exact conformal invariance demands also the presence of a non-trivial metric and antisymmetric tensor (induced by magnetic field). The model is invariant under target space duality in a compact Kaluza-Klein direction introduced to couple the magnetic field. Like open string theory in a constant gauge field, or closed string theory on a torus, this model can be straightforwardly quantized and solved with its spectrum of states and partition function explicitly computed. Above some critical value of the magnetic field an infinite number of states become tachyonic, suggesting a presence of phase transition. We also construct heterotic string generalisations of this bosonic model in which the constant magnetic field is embedded either in the Kaluza-Klein or internal gauge group sector.We consider a simple model describing a closed bosonic string in a constant magnetic field. Exact conformal invariance demands also the presence of a non-trivial metric and antisymmetric tensor (induced by the magnetic field). The model is invariant under target space duality in a compact Kaluza-Klein direction introduced to couple the magnetic field. Like open string theory in a constant gauge field, or closed string theory on a torus, this model can be straightforwardly quantised and solved with its spectrum of states and partition function explicitly computed. Above some critical value of the magnetic field an infinite number of states become tachyonic, suggesting a presence of phase transition. We also construct heterotic string generalisations of this bosonic model in which the constant magnetic field is embedded either in the Kaluza-Klein or internal gauge group sector.hep-th/9411099CERN-TH-7494-94IMPERIAL-TP-94-95-3CERN-TH-7494-94IMPERIAL-TP-94-95-3oai:cds.cern.ch:2721261994-11-14
spellingShingle Particle Physics - Theory
Particle Physics - Theory
Russo, J.G.
Tseytlin, Arkady A.
Constant magnetic field in closed string theory: an exactly solvable model
title Constant magnetic field in closed string theory: an exactly solvable model
title_full Constant magnetic field in closed string theory: an exactly solvable model
title_fullStr Constant magnetic field in closed string theory: an exactly solvable model
title_full_unstemmed Constant magnetic field in closed string theory: an exactly solvable model
title_short Constant magnetic field in closed string theory: an exactly solvable model
title_sort constant magnetic field in closed string theory: an exactly solvable model
topic Particle Physics - Theory
Particle Physics - Theory
url https://dx.doi.org/10.1016/0550-3213(95)00091-6
http://cds.cern.ch/record/272126
work_keys_str_mv AT russojg constantmagneticfieldinclosedstringtheoryanexactlysolvablemodel
AT tseytlinarkadya constantmagneticfieldinclosedstringtheoryanexactlysolvablemodel