Please use this identifier to cite or link to this item: http://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/4301
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dc.contributor.authorANANTH, SUDARSHANen_US
dc.date.accessioned2019-12-24T12:30:57Z
dc.date.available2019-12-24T12:30:57Z
dc.date.issued2009-08en_US
dc.identifier.citationFortschritte der Physik Progress of Physics, 57(9), 857-861.en_US
dc.identifier.issn0015-8208en_US
dc.identifier.issn1521-3978en_US
dc.identifier.urihttp://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/4301-
dc.identifier.urihttps://doi.org/10.1002/prop.200900062en_US
dc.description.abstractThe pure gravity Lagrangian can be written as the “square” of the pure Yang‐Mills Lagrangian to second order in coupling constants. This paper uses this form of the gravity Lagrangian as a starting point to arrive at a compact light‐cone superspace Lagrangian for 𝒩 = 8 supergravity to order κ2.en_US
dc.language.isoenen_US
dc.publisherWileyen_US
dc.subjectGravity squareen_US
dc.subjectYang?Millsen_US
dc.subject8 Supergravityen_US
dc.subjectCompact light?cone superspaceen_US
dc.subject2009en_US
dc.titleGravity as the square of Yang‐Mills: implications for 𝒩 = 8 supergravityen_US
dc.typeArticleen_US
dc.contributor.departmentDept. of Physicsen_US
dc.identifier.sourcetitleFortschritte der Physik Progress of Physicsen_US
dc.publication.originofpublisherForeignen_US
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