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String beta function equations from c=1 matrix model

We derive the \sigma-model tachyon \beta-function equation of 2-dimensional string theory, in the background of flat space and linear dilaton, working entirely within the c=1 matrix model. The tachyon \beta-function equation is satisfied by a \underbar{nonlocal} and \underbar{nonlinear} combination...

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Detalles Bibliográficos
Autores principales: Dhar, Avinash, Mandal, Gautam, Wadia, Spenta R.
Lenguaje:eng
Publicado: 1995
Materias:
Acceso en línea:https://dx.doi.org/10.1016/0550-3213(95)00319-N
http://cds.cern.ch/record/279130
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author Dhar, Avinash
Mandal, Gautam
Wadia, Spenta R.
author_facet Dhar, Avinash
Mandal, Gautam
Wadia, Spenta R.
author_sort Dhar, Avinash
collection CERN
description We derive the \sigma-model tachyon \beta-function equation of 2-dimensional string theory, in the background of flat space and linear dilaton, working entirely within the c=1 matrix model. The tachyon \beta-function equation is satisfied by a \underbar{nonlocal} and \underbar{nonlinear} combination of the (massless) scalar field of the matrix model. We discuss the possibility of describing the `discrete states' as well as other possible gravitational and higher tensor backgrounds of 2-dimensional string theory within the c=1 matrix model. We also comment on the realization of the W-infinity symmetry of the matrix model in the string theory. The present work reinforces the viewpoint that a nonlocal (and nonlinear) transform is required to extract the space-time physics of 2-dimensional string theory from the c=1 matrix model.
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spelling cern-2791302023-03-14T18:56:23Zdoi:10.1016/0550-3213(95)00319-Nhttp://cds.cern.ch/record/279130engDhar, AvinashMandal, GautamWadia, Spenta R.String beta function equations from c=1 matrix modelParticle Physics - TheoryWe derive the \sigma-model tachyon \beta-function equation of 2-dimensional string theory, in the background of flat space and linear dilaton, working entirely within the c=1 matrix model. The tachyon \beta-function equation is satisfied by a \underbar{nonlocal} and \underbar{nonlinear} combination of the (massless) scalar field of the matrix model. We discuss the possibility of describing the `discrete states' as well as other possible gravitational and higher tensor backgrounds of 2-dimensional string theory within the c=1 matrix model. We also comment on the realization of the W-infinity symmetry of the matrix model in the string theory. The present work reinforces the viewpoint that a nonlocal (and nonlinear) transform is required to extract the space-time physics of 2-dimensional string theory from the c=1 matrix model.We derive the $\sigma$-model tachyon $\beta$-function equation of 2-dimensional string theory, in the background of flat space and linear dilaton, working entirely within the $c=1$ matrix model. The tachyon $\beta$-function equation is satisfied by a \underbar{nonlocal} and \underbar{nonlinear} combination of the (massless) scalar field of the matrix model. We discuss the possibility of describing the `discrete states' as well as other possible gravitational and higher tensor backgrounds of 2-dimensional string theory within the $c=1$ matrix model. We also comment on the realization of the $W$-infinity symmetry of the matrix model in the string theory. The present work reinforces the viewpoint that a nonlocal (and nonlinear) transform is required to extract the space-time physics of 2-dimensional string theory from the $c=1$ matrix model.We derive the σ-model tachyon β-function equation of 2-dimensional string theory, in the background of flat space and linear dilaton, working entirely within the c = 1 matrix model. The tachyon β-function equation is satisfied by a nonlocal and nonlinear combination of the (massless) scalar field of the matrix model. We discuss the possibility of describing the ‘discrete states’ as well as other possible gravitational and higher tensor backgrounds of 2-dimensional string theory within the c = 1 matrix model. We also comment on the realization of the W-infinity symmetry of the matrix model in the string theory. The present work reinforces the viewpoint that a nonlocal (and nonlinear) transform is required to extract the space-time physics of 2-dimensional string theory from the c = 1 matrix model.hep-th/9503172CERN-TH-95-69CERN-TH-95-069TIFR-TH-95-11CERN-TH-95-69TIFR-TH-95-11oai:cds.cern.ch:2791301995-03-24
spellingShingle Particle Physics - Theory
Dhar, Avinash
Mandal, Gautam
Wadia, Spenta R.
String beta function equations from c=1 matrix model
title String beta function equations from c=1 matrix model
title_full String beta function equations from c=1 matrix model
title_fullStr String beta function equations from c=1 matrix model
title_full_unstemmed String beta function equations from c=1 matrix model
title_short String beta function equations from c=1 matrix model
title_sort string beta function equations from c=1 matrix model
topic Particle Physics - Theory
url https://dx.doi.org/10.1016/0550-3213(95)00319-N
http://cds.cern.ch/record/279130
work_keys_str_mv AT dharavinash stringbetafunctionequationsfromc1matrixmodel
AT mandalgautam stringbetafunctionequationsfromc1matrixmodel
AT wadiaspentar stringbetafunctionequationsfromc1matrixmodel