Please use this identifier to cite or link to this item: http://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/1451
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dc.contributor.authorJAIN, SACHINen_US
dc.contributor.authorChoudhury, Sayantan et al.en_US
dc.date.accessioned2018-12-28T06:58:08Z
dc.date.available2018-12-28T06:58:08Z
dc.date.issued2018-11en_US
dc.identifier.citationJournal of High Energy Physics, No.11.en_US
dc.identifier.issn1029-8479en_US
dc.identifier.urihttp://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/1451-
dc.identifier.urihttps://doi.org/10.1007/JHEP11(2018)177en_US
dc.description.abstractIt has been conjectured that fermions minimally coupled to a Chern-Simons gauge field define a conformal field theory (CFT) that is level-rank dual to Chern-Simons gauged Wilson-Fisher Bosons. The CFTs in question admit relevant deformations parametrized by a real mass. When the mass deformation is positive, the duality of the two deformed theories has previously been checked in detail in the large Nlimit by comparing explicit all orders results on both sides of the duality. In this paper we perform a similar check for the case of negative mass deformations. In this case the bosonic field condenses triggering the Higgs mechanism. The effective excitations in this phase are massiveWbosons. By summing all leading large N graphs involving theseWbosons we find an all orders (in the t Hooft coupling) result for the thermal free energy of the bosonic theory in the condensed phase. Our final answer perfectly matches the previously obtained fermionic free energy under the conjectured duality map.en_US
dc.language.isoenen_US
dc.publisherSpringer Natureen_US
dc.subject1/N Expansionen_US
dc.subjectChern-Simons Theoriesen_US
dc.subjectTOC-DEC-2018en_US
dc.subject2018en_US
dc.titleBose-Fermi Chern-Simons dualities in the Higgsed phaseen_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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