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Dual models with SL(2, C) symmetry

Making use of homogeneous space techniques, the authors construct a class of dual models, which is a generalization of the Virasoro- Shapiro type of model. The integrand in the integral representation for the N-point function depends not only on the modulus of the distances between two-dimensional K...

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Detalles Bibliográficos
Autores principales: Brink, L, Kihlberg, A
Lenguaje:eng
Publicado: 1972
Materias:
Acceso en línea:https://dx.doi.org/10.1016/0550-3213(72)90081-8
http://cds.cern.ch/record/875641
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author Brink, L
Kihlberg, A
author_facet Brink, L
Kihlberg, A
author_sort Brink, L
collection CERN
description Making use of homogeneous space techniques, the authors construct a class of dual models, which is a generalization of the Virasoro- Shapiro type of model. The integrand in the integral representation for the N-point function depends not only on the modulus of the distances between two-dimensional Koba-Nielsen variables, but also on the corresponding phases. This is in fact the most general SL(2, C) invariant amplitude that can be constructed using complex integration variables. The extra phase factors in the integrand provide a possible means of avoiding tachyons both as external particles and as intermediate states in the amplitude. When factorized in a simple- minded fashion the intercepts are fixed to be integers. Although the external particles can be chosen not to be tachyons, such states appear as intermediate states. Within this factorization one can show that there are gauge conditions for the amplitude that can provide a ghostkilling mechanism. (19 refs).
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spelling cern-8756412019-09-30T06:29:59Zdoi:10.1016/0550-3213(72)90081-8http://cds.cern.ch/record/875641engBrink, LKihlberg, ADual models with SL(2, C) symmetryParticle Physics - TheoryMaking use of homogeneous space techniques, the authors construct a class of dual models, which is a generalization of the Virasoro- Shapiro type of model. The integrand in the integral representation for the N-point function depends not only on the modulus of the distances between two-dimensional Koba-Nielsen variables, but also on the corresponding phases. This is in fact the most general SL(2, C) invariant amplitude that can be constructed using complex integration variables. The extra phase factors in the integrand provide a possible means of avoiding tachyons both as external particles and as intermediate states in the amplitude. When factorized in a simple- minded fashion the intercepts are fixed to be integers. Although the external particles can be chosen not to be tachyons, such states appear as intermediate states. Within this factorization one can show that there are gauge conditions for the amplitude that can provide a ghostkilling mechanism. (19 refs).CERN-TH-1502oai:cds.cern.ch:8756411972
spellingShingle Particle Physics - Theory
Brink, L
Kihlberg, A
Dual models with SL(2, C) symmetry
title Dual models with SL(2, C) symmetry
title_full Dual models with SL(2, C) symmetry
title_fullStr Dual models with SL(2, C) symmetry
title_full_unstemmed Dual models with SL(2, C) symmetry
title_short Dual models with SL(2, C) symmetry
title_sort dual models with sl(2, c) symmetry
topic Particle Physics - Theory
url https://dx.doi.org/10.1016/0550-3213(72)90081-8
http://cds.cern.ch/record/875641
work_keys_str_mv AT brinkl dualmodelswithsl2csymmetry
AT kihlberga dualmodelswithsl2csymmetry