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Superstrings with new supersymmetry in (9,2) and (10,2) dimensions

We construct superstring theories that obey the new supersymmetry algebra {Q_a , Q_b}=\gamma_{ab}^{mn} P_{1m} P_{2n}, in a Green-Schwarz formalism, with kappa supersymmetry also of the new type. The superstring is in a system with a superparticle so that their total momenta are $P_{2n},P_{1m}$ respe...

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Detalles Bibliográficos
Autores principales: Bars, Itzhak, Deliduman, Cemsinan
Lenguaje:eng
Publicado: 1997
Materias:
Acceso en línea:https://dx.doi.org/10.1103/PhysRevD.56.6579
http://cds.cern.ch/record/330834
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author Bars, Itzhak
Deliduman, Cemsinan
author_facet Bars, Itzhak
Deliduman, Cemsinan
author_sort Bars, Itzhak
collection CERN
description We construct superstring theories that obey the new supersymmetry algebra {Q_a , Q_b}=\gamma_{ab}^{mn} P_{1m} P_{2n}, in a Green-Schwarz formalism, with kappa supersymmetry also of the new type. The superstring is in a system with a superparticle so that their total momenta are $P_{2n},P_{1m}$ respectively. The system is covariant and critical in (10,2) dimensions if the particle is massless and in (9,2) dimensions if the particle is massive. Both the superstring and superparticle have coordinates with two timelike dimensions but each behaves effectively as if they have a single timelike dimension. This is due to gauge symmetries and associated constraints. We show how to generalize the gauge principle to more intricate systems containing two parts, 1 and 2. Each part contains interacting constituents, such as p-branes, and each part behaves effectively as if they have one timelike coordinate, although the full system has two timelike coordinates. The examples of two superparticles, and of a superparticle and a superstring, discussed in more detail are a special cases of such a generalized interacting system.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1997
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spelling cern-3308342023-03-14T17:09:39Zdoi:10.1103/PhysRevD.56.6579http://cds.cern.ch/record/330834engBars, ItzhakDeliduman, CemsinanSuperstrings with new supersymmetry in (9,2) and (10,2) dimensionsParticle Physics - TheoryWe construct superstring theories that obey the new supersymmetry algebra {Q_a , Q_b}=\gamma_{ab}^{mn} P_{1m} P_{2n}, in a Green-Schwarz formalism, with kappa supersymmetry also of the new type. The superstring is in a system with a superparticle so that their total momenta are $P_{2n},P_{1m}$ respectively. The system is covariant and critical in (10,2) dimensions if the particle is massless and in (9,2) dimensions if the particle is massive. Both the superstring and superparticle have coordinates with two timelike dimensions but each behaves effectively as if they have a single timelike dimension. This is due to gauge symmetries and associated constraints. We show how to generalize the gauge principle to more intricate systems containing two parts, 1 and 2. Each part contains interacting constituents, such as p-branes, and each part behaves effectively as if they have one timelike coordinate, although the full system has two timelike coordinates. The examples of two superparticles, and of a superparticle and a superstring, discussed in more detail are a special cases of such a generalized interacting system.We construct superstring theories that obey the new supersymmetry algebra {Q_a , Q_b}=\gamma_{ab}^{mn} P_{1m} P_{2n}, in a Green-Schwarz formalism, with kappa supersymmetry also of the new type. The superstring is in a system with a superparticle so that their total momenta are $P_{2n},P_{1m}$ respectively. The system is covariant and critical in (10,2) dimensions if the particle is massless and in (9,2) dimensions if the particle is massive. Both the superstring and superparticle have coordinates with two timelike dimensions but each behaves effectively as if they have a single timelike dimension. This is due to gauge symmetries and associated constraints. We show how to generalize the gauge principle to more intricate systems containing two parts, 1 and 2. Each part contains interacting constituents, such as p-branes, and each part behaves effectively as if they have one timelike coordinate, although the full system has two timelike coordinates. The examples of two superparticles, and of a superparticle and a superstring, discussed in more detail are a special cases of such a generalized interacting system.hep-th/9707215CERN-TH-97-181USC-97-HEP-B5CERN-TH-97-181USC-97-HEP-B-5oai:cds.cern.ch:3308341997-07-28
spellingShingle Particle Physics - Theory
Bars, Itzhak
Deliduman, Cemsinan
Superstrings with new supersymmetry in (9,2) and (10,2) dimensions
title Superstrings with new supersymmetry in (9,2) and (10,2) dimensions
title_full Superstrings with new supersymmetry in (9,2) and (10,2) dimensions
title_fullStr Superstrings with new supersymmetry in (9,2) and (10,2) dimensions
title_full_unstemmed Superstrings with new supersymmetry in (9,2) and (10,2) dimensions
title_short Superstrings with new supersymmetry in (9,2) and (10,2) dimensions
title_sort superstrings with new supersymmetry in (9,2) and (10,2) dimensions
topic Particle Physics - Theory
url https://dx.doi.org/10.1103/PhysRevD.56.6579
http://cds.cern.ch/record/330834
work_keys_str_mv AT barsitzhak superstringswithnewsupersymmetryin92and102dimensions
AT delidumancemsinan superstringswithnewsupersymmetryin92and102dimensions