dc.contributor.author |
JAIN, SACHIN |
en_US |
dc.contributor.author |
Choudhury, Sayantan et al. |
en_US |
dc.date.accessioned |
2018-12-28T06:58:08Z |
|
dc.date.available |
2018-12-28T06:58:08Z |
|
dc.date.issued |
2018-11 |
en_US |
dc.identifier.citation |
Journal of High Energy Physics, No.11. |
en_US |
dc.identifier.issn |
1029-8479 |
en_US |
dc.identifier.uri |
http://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/1451 |
|
dc.identifier.uri |
https://doi.org/10.1007/JHEP11(2018)177 |
en_US |
dc.description.abstract |
It 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.iso |
en |
en_US |
dc.publisher |
Springer Nature |
en_US |
dc.subject |
1/N Expansion |
en_US |
dc.subject |
Chern-Simons Theories |
en_US |
dc.subject |
TOC-DEC-2018 |
en_US |
dc.subject |
2018 |
en_US |
dc.title |
Bose-Fermi Chern-Simons dualities in the Higgsed phase |
en_US |
dc.type |
Article |
en_US |
dc.contributor.department |
Dept. of Physics |
en_US |
dc.identifier.sourcetitle |
Journal of High Energy Physics |
en_US |
dc.publication.originofpublisher |
Foreign |
en_US |