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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...
Autores principales: | , |
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Lenguaje: | eng |
Publicado: |
1997
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Acceso en línea: | https://dx.doi.org/10.1103/PhysRevD.56.6579 http://cds.cern.ch/record/330834 |
_version_ | 1780891110716997632 |
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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. |
id | cern-330834 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 1997 |
record_format | invenio |
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 |