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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...
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Lenguaje: | eng |
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2005
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Acceso en línea: | https://dx.doi.org/10.1016/j.physletb.2005.04.001 http://cds.cern.ch/record/822120 |
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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 |