Please use this identifier to cite or link to this item: http://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/1675
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dc.contributor.authorAkshay, Y. S.en_US
dc.contributor.authorANANTH, SUDARSHANen_US
dc.date.accessioned2019-02-14T05:02:29Z
dc.date.available2019-02-14T05:02:29Z
dc.date.issued2014-01en_US
dc.identifier.citationJournal of Physics A: Mathematical and Theoretical, 47(4), 045401.en_US
dc.identifier.issn1751-8113en_US
dc.identifier.issn1751-8121en_US
dc.identifier.urihttp://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/1675-
dc.identifier.urihttps://doi.org/10.1088/1751-8113/47/4/045401en_US
dc.description.abstractBased purely on symmetry considerations, we derive the following result: in momentum space, the cubic term in the Lagrangian for a field of spin λ is equal to the cubic term in Yang–Mills theory, raised to the power λ. This result is valid for all λ for Lagrangians that contain a cubic interaction vertex involving three spin λ fields, in four-dimensional flat spacetime. For λ = 3, we present an additional derivation of this result.en_US
dc.language.isoenen_US
dc.publisherIOP Publishingen_US
dc.subjectCubic interactionen_US
dc.subjectHigher spin theoriesen_US
dc.subjectHigher spin fieldsen_US
dc.subjectGravity and Yang Millsen_US
dc.subject2014en_US
dc.titleCubic interaction vertices in higher spin theoriesen_US
dc.typeArticleen_US
dc.contributor.departmentDept. of Physicsen_US
dc.identifier.sourcetitleJournal of Physics A: Mathematical and Theoreticalen_US
dc.publication.originofpublisherForeignen_US
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