Massive and massless gauge fields of any spin and symmetry
Identifieur interne : 001E91 ( Istex/Curation ); précédent : 001E90; suivant : 001E92Massive and massless gauge fields of any spin and symmetry
Auteurs : F. Hussain [Allemagne, Pakistan] ; G. Thompson [Italie, France] ; P. D. JarvisSource :
- Physics Letters B [ 0370-2693 ] ; 1989.
English descriptors
- KwdEn :
- Algebra, Antisymmetric, Antisymmetric tensors, Auxiliary fields, Bosonic, Brst, Brst operator, Covariant operators, Cubic interaction, Dimensional reduction, Double trace, Double trace condition, Double trace constraint, Fermionic fields, Field content, Fock space, Gauge parameter, Grassmann covariant operators, Interesting possibility, Mass dimensions, Mass term, Massive theories, Massive theory, Massless, Massless action, Massless gauge fields, Massless particles, Massless theory, Number physics letters, Number physics lettersb, Permutation symmetry, Phys, Previous results, String field theory, String theory, Symmetric tensors, Tensor, Theoretical physics.
- Teeft :
- Algebra, Antisymmetric, Antisymmetric tensors, Auxiliary fields, Bosonic, Brst, Brst operator, Covariant operators, Cubic interaction, Dimensional reduction, Double trace, Double trace condition, Double trace constraint, Fermionic fields, Field content, Fock space, Gauge parameter, Grassmann covariant operators, Interesting possibility, Mass dimensions, Mass term, Massive theories, Massive theory, Massless, Massless action, Massless gauge fields, Massless particles, Massless theory, Number physics letters, Number physics lettersb, Permutation symmetry, Phys, Previous results, String field theory, String theory, Symmetric tensors, Tensor, Theoretical physics.
Abstract
Abstract: An analysis of the BRST approach to massive and massless gauge fields of any spin and symmetry is presented. Previous results on massless gauge fields are extended to totally antisymmetric massless tensors and Kähler-Dirac particles. Two methods for arriving at a BRST invariant, massive theory from the corresponding massless one are discussed. The first allows for an interpretation in terms of dimensional reduction, while the second keeps the BRST operator of the massless theory, but employs gauge invariant fields.
Url:
DOI: 10.1016/0370-2693(89)91384-1
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P. D. Jarvis<affiliation><mods:affiliation>Department of Physics, University of Tasmania, P.O. Box 252C, Hobart, Australia 7001</mods:affiliation>
<wicri:noCountry code="subField">7001</wicri:noCountry>
</affiliation>
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<term>Brst</term>
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<term>Brst operator</term>
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<front><div type="abstract" xml:lang="en">Abstract: An analysis of the BRST approach to massive and massless gauge fields of any spin and symmetry is presented. Previous results on massless gauge fields are extended to totally antisymmetric massless tensors and Kähler-Dirac particles. Two methods for arriving at a BRST invariant, massive theory from the corresponding massless one are discussed. The first allows for an interpretation in terms of dimensional reduction, while the second keeps the BRST operator of the massless theory, but employs gauge invariant fields.</div>
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