Please use this identifier to cite or link to this item: http://hdl.handle.net/123456789/1985
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dc.contributor.authorKrishna, S.-
dc.date.accessioned2020-11-20T09:19:52Z-
dc.date.available2020-11-20T09:19:52Z-
dc.date.issued2017-
dc.identifier.citationEuropean Physical Journal C, 77 (6)en_US
dc.identifier.other10.1140/epjc/s10052-017-4954-y-
dc.identifier.urihttps://link.springer.com/article/10.1140/epjc/s10052-017-4954-y-
dc.identifier.urihttp://hdl.handle.net/123456789/1985-
dc.descriptionOnly IISERM authors are available in the record.-
dc.description.abstractWe discuss the complete sets of the off-shell nilpotent (i.e. ๐‘ 2(๐‘Ž)๐‘=0) and absolutely anticommuting (i.e. ๐‘ ๐‘๐‘ ๐‘Ž๐‘+๐‘ ๐‘Ž๐‘๐‘ ๐‘=0) Becchiโ€“Rouetโ€“Storaโ€“Tyutin (BRST) (๐‘ ๐‘) and anti-BRST (๐‘ ๐‘Ž๐‘) symmetries for the (3+1)-dimensional (4D) gauge-invariant massive 2-form theory within the framework of an augmented superfield approach to the BRST formalism. In this formalism, we obtain the coupled (but equivalent) Lagrangian densities which respect both BRST and anti-BRST symmetries on the constrained hypersurface defined by the Curciโ€“Ferrari type conditions. The absolute anticommutativity property of the (anti-) BRST transformations (and corresponding generators) is ensured by the existence of the Curciโ€“Ferrari type conditions which emerge very naturally in this formalism. Furthermore, the gauge-invariant restriction plays a decisive role in deriving the proper (anti-) BRST transformations for the Stรผckelberg-like vector field.en_US
dc.language.isoen_USen_US
dc.publisherSpringeren_US
dc.subjectoff-shell nilpotent (i.e. ๐‘ 2(๐‘Ž)๐‘=0)en_US
dc.subjectanticommutingen_US
dc.subject๐‘ ๐‘๐‘ ๐‘Ž๐‘+๐‘ ๐‘Ž๐‘๐‘ ๐‘=0en_US
dc.subjectBecchiโ€“Rouetโ€“Storaโ€“Tyutin (BRST)en_US
dc.titleAugmented superfield approach to gauge-invariant massive 2-form theoryen_US
dc.typeArticleen_US
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