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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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Lenguaje: | eng |
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1981
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Acceso en línea: | http://cds.cern.ch/record/877991 |
_version_ | 1780907921919442944 |
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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 |