Cargando…

Tensionless strings, correspondence with SO(D,D) sigma model

String theory with perimeter action is tensionless by its geometrical nature and has pure massless spectrum of higher spin gauge particles. I demonstrate that liner transformation of the world-sheet fields defines a map to the SO(D,D) sigma model equipped by additional Abelian constraint, which brea...

Descripción completa

Detalles Bibliográficos
Autor principal: Savvidy, G.
Lenguaje:eng
Publicado: 2005
Materias:
Acceso en línea:https://dx.doi.org/10.1016/j.physletb.2005.04.001
http://cds.cern.ch/record/822120
_version_ 1780905574463963136
author Savvidy, G.
author_facet Savvidy, G.
author_sort Savvidy, G.
collection CERN
description String theory with perimeter action is tensionless by its geometrical nature and has pure massless spectrum of higher spin gauge particles. I demonstrate that liner transformation of the world-sheet fields defines a map to the SO(D,D) sigma model equipped by additional Abelian constraint, which breaks SO(D,D) to a diagonal SO(1,D-1). The effective tension is equal to the square of the dimensional coupling constant of the perimeter action. This correspondence allows to view the perimeter action as a "square root" of the Nambu-Goto area action. The aforementioned map between tensionless strings and SO(D,D) sigma model allows to introduce the vertex operators in full analogy with the standard string theory and to confirm the form of the vertex operators introduced earlier.
id cern-822120
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2005
record_format invenio
spelling cern-8221202023-03-14T18:17:35Zdoi:10.1016/j.physletb.2005.04.001http://cds.cern.ch/record/822120engSavvidy, G.Tensionless strings, correspondence with SO(D,D) sigma modelParticle Physics - TheoryString theory with perimeter action is tensionless by its geometrical nature and has pure massless spectrum of higher spin gauge particles. I demonstrate that liner transformation of the world-sheet fields defines a map to the SO(D,D) sigma model equipped by additional Abelian constraint, which breaks SO(D,D) to a diagonal SO(1,D-1). The effective tension is equal to the square of the dimensional coupling constant of the perimeter action. This correspondence allows to view the perimeter action as a "square root" of the Nambu-Goto area action. The aforementioned map between tensionless strings and SO(D,D) sigma model allows to introduce the vertex operators in full analogy with the standard string theory and to confirm the form of the vertex operators introduced earlier.String theory with perimeter action is tensionless by its geometrical nature and has pure massless spectrum of higher spin gauge particles. I demonstrate that liner transformation of the world-sheet fields defines a map to the SO(D,D) sigma model equipped by additional Abelian constraint, which breaks SO(D,D) to a diagonal SO(1,D-1). The effective tension is equal to the square of the dimensional coupling constant of the perimeter action. This correspondence allows to view the perimeter action as a square root of the Nambu-Goto area action. The aforementioned map between tensionless strings and SO(D,D) sigma model allows to introduce the vertex operators in full analogy with the standard string theory and to confirm the form of the vertex operators introduced earlier.String theory with perimeter action is tensionless by its geometrical nature and has pure massless spectrum of higher spin gauge particles. I demonstrate that liner transformation of the world-sheet fields defines a map to the SO(D,D) sigma model equipped by additional Abelian constraint, which breaks SO(D,D) to a diagonal SO(1,D-1). The effective tension is equal to the square of the dimensional coupling constant of the perimeter action. This correspondence allows to view the perimeter action as a square root of the Nambu-Goto area action. The aforementioned map between tensionless strings and SO(D,D) sigma model allows to introduce the vertex operators in full analogy with the standard string theory and to confirm the form of the vertex operators introduced earlier.The string theory with perimeter action is tensionless by its geometrical nature and has a pure massless spectrum of higher spin gauge particles. I demonstrate that the linear transformation of the world-sheet fields defines a map to the SO(D,D) sigma-model equipped by additional Abelian constraint, which breaks SO(D,D) to a diagonal SO(1,D−1) . The effective tension is equal to the square of the dimensional coupling constant of the perimeter action. This correspondence allows to view the perimeter action as a “square root” of the Nambu–Goto area action. The aforementioned correspondence between tensionless strings and SO(D,D) sigma-model allows to introduce vertex operators in full analogy with the standard string theory and to confirm the form of the vertex operators introduced earlier, the value of the intercept a=1 and the critical dimension D=13 .hep-th/0502114CERN-PH-TH-2005-024NRCPS-HE-2005-13CERN-PH-TH-2005-024NRCPS-HE-2005-13oai:cds.cern.ch:8221202005-02-12
spellingShingle Particle Physics - Theory
Savvidy, G.
Tensionless strings, correspondence with SO(D,D) sigma model
title Tensionless strings, correspondence with SO(D,D) sigma model
title_full Tensionless strings, correspondence with SO(D,D) sigma model
title_fullStr Tensionless strings, correspondence with SO(D,D) sigma model
title_full_unstemmed Tensionless strings, correspondence with SO(D,D) sigma model
title_short Tensionless strings, correspondence with SO(D,D) sigma model
title_sort tensionless strings, correspondence with so(d,d) sigma model
topic Particle Physics - Theory
url https://dx.doi.org/10.1016/j.physletb.2005.04.001
http://cds.cern.ch/record/822120
work_keys_str_mv AT savvidyg tensionlessstringscorrespondencewithsoddsigmamodel