Please use this identifier to cite or link to this item: http://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/5519
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dc.contributor.authorANANTH, SUDARSHANen_US
dc.contributor.authorMalcha, Hannesen_US
dc.contributor.authorPANDEY, CHETANen_US
dc.contributor.authorPANT, SAURABHen_US
dc.date.accessioned2021-01-15T05:45:29Z
dc.date.available2021-01-15T05:45:29Z
dc.date.issued2021-01en_US
dc.identifier.citationPhysical Review D, 103(2), 025010.en_US
dc.identifier.issn2470-0029en_US
dc.identifier.issn2470-0010en_US
dc.identifier.urihttp://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/5519
dc.identifier.urihttps://doi.org/10.1103/PhysRevD.103.025010en_US
dc.description.abstractSupersymmetric Yang–Mills theory is formulated in six dimensions, without the use of anticommuting variables. This is achieved using a new Nicolai map, to third order in the coupling constant. This is the second such map in six dimensions and highlights a potential ambiguity in the formalism.en_US
dc.language.isoenen_US
dc.publisherAmerican Physical Societyen_US
dc.subjectYang–Mills theoryen_US
dc.subjectSupersymmetryen_US
dc.subject2021-JAN-WEEK2en_US
dc.subjectTOC-JAN-2021en_US
dc.subject2021en_US
dc.titleSupersymmetric Yang-Mills theory in D=6 without anticommuting variablesen_US
dc.typeArticleen_US
dc.contributor.departmentDept. of Physicsen_US
dc.identifier.sourcetitlePhysical Review Den_US
dc.publication.originofpublisherForeignen_US
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