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Minimal geometric superspace approach to N=1 supergravity

Describes an approach to N=1 supergravity which is both geometric (i.ee. formulated in superspace) and minimal. Its main features are: 1) It is based on a clear and simple geometric picture; 2) the gauge group is the smallest possible; 3) the only independent dynamical variable is the axial superfie...

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Autor principal: Sokatchev, Emery S
Lenguaje:eng
Publicado: 1981
Materias:
Acceso en línea:http://cds.cern.ch/record/877991
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author Sokatchev, Emery S
author_facet Sokatchev, Emery S
author_sort Sokatchev, Emery S
collection CERN
description Describes an approach to N=1 supergravity which is both geometric (i.ee. formulated in superspace) and minimal. Its main features are: 1) It is based on a clear and simple geometric picture; 2) the gauge group is the smallest possible; 3) the only independent dynamical variable is the axial superfield (SF) H/sup m/( chi , theta , theta ); 4) the components of the torsions T/sub AB//sup C/ and curvature R/sub ABC//sup D/ tensors are expressed in terms of H/sup m/; 5) the action principle is straightforward, i.e. the equations of motion are directly obtained by varying H/sup m/ in the action; 6) a special gauge (called 'normal gauge') can be introduced in which a lot of the derivatives of H/sup m/ vanish at a given point in superspace. (22 refs).
id cern-877991
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1981
record_format invenio
spelling cern-8779912019-09-30T06:29:59Zhttp://cds.cern.ch/record/877991engSokatchev, Emery SMinimal geometric superspace approach to N=1 supergravityGeneral Relativity and CosmologyDescribes an approach to N=1 supergravity which is both geometric (i.ee. formulated in superspace) and minimal. Its main features are: 1) It is based on a clear and simple geometric picture; 2) the gauge group is the smallest possible; 3) the only independent dynamical variable is the axial superfield (SF) H/sup m/( chi , theta , theta ); 4) the components of the torsions T/sub AB//sup C/ and curvature R/sub ABC//sup D/ tensors are expressed in terms of H/sup m/; 5) the action principle is straightforward, i.e. the equations of motion are directly obtained by varying H/sup m/ in the action; 6) a special gauge (called 'normal gauge') can be introduced in which a lot of the derivatives of H/sup m/ vanish at a given point in superspace. (22 refs).oai:cds.cern.ch:8779911981
spellingShingle General Relativity and Cosmology
Sokatchev, Emery S
Minimal geometric superspace approach to N=1 supergravity
title Minimal geometric superspace approach to N=1 supergravity
title_full Minimal geometric superspace approach to N=1 supergravity
title_fullStr Minimal geometric superspace approach to N=1 supergravity
title_full_unstemmed Minimal geometric superspace approach to N=1 supergravity
title_short Minimal geometric superspace approach to N=1 supergravity
title_sort minimal geometric superspace approach to n=1 supergravity
topic General Relativity and Cosmology
url http://cds.cern.ch/record/877991
work_keys_str_mv AT sokatchevemerys minimalgeometricsuperspaceapproachton1supergravity