Please use this identifier to cite or link to this item: http://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/6476
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dc.contributor.authorJAIN, SACHINen_US
dc.contributor.authorJOHN, RENJAN RAJANen_US
dc.date.accessioned2021-12-20T10:00:08Z
dc.date.available2021-12-20T10:00:08Z
dc.date.issued2021-12en_US
dc.identifier.citationJournal of High Energy Physics, 2021(12), 67.en_US
dc.identifier.issn1029-8479en_US
dc.identifier.urihttp://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/6476
dc.identifier.urihttps://doi.org/10.1007/JHEP12(2021)067en_US
dc.description.abstractIn this paper we relate the parity-odd part of two and three point correlation functions in theories with exactly conserved or weakly broken higher spin symmetries to the parity-even part which can be computed from free theories. We also comment on higher point functions.The well known connection of CFT correlation functions with de-Sitter amplitudes in one higher dimension implies a relation between parity-even and parity-odd amplitudes calculated using non-minimal interactions such as W3 and W2W~. In the flat-space limit this implies a relation between parity-even and parity-odd parts of flat-space scattering amplitudes.en_US
dc.language.isoenen_US
dc.publisherSpringer Natureen_US
dc.subjectConformal Field Theoryen_US
dc.subjectChern-Simons Theoriesen_US
dc.subject2021-DEC-WEEK3en_US
dc.subjectTOC-DEC-2021en_US
dc.subject2021en_US
dc.titleRelation between parity-even and parity-odd CFT correlation functions in three dimensionsen_US
dc.typeArticleen_US
dc.contributor.departmentDept. of Physicsen_US
dc.identifier.sourcetitleJournal of High Energy Physicsen_US
dc.publication.originofpublisherForeignen_US
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