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dc.contributor.authorAndersen, Jens Oluf
dc.contributor.authorAdhikari, Prabal
dc.date.accessioned2017-12-19T14:54:13Z
dc.date.available2017-12-19T14:54:13Z
dc.date.created2017-03-27T17:23:04Z
dc.date.issued2017
dc.identifier.issn0556-2821
dc.identifier.urihttp://hdl.handle.net/11250/2473061
dc.description.abstractIn this paper, we study the possibility of an inhomogeneous quark condensate in the (1 þ 1)-dimensional Nambu-Jona-Lasinio model in the large-Nc limit at finite temperature T and quark chemical potential μ using dimensional regularization. The phase diagram in the μ–T plane is mapped out. At zero temperature, an inhomogeneous phase with a chiral-density wave exists for μ > μc, where μc is a critical chemical potential. Performing a Ginzburg-Landau analysis, we show that in the chiral limit, the tricritical point and the Lifschitz point coincide. We also consider the competition between a chiral-density wave and a constant pion condensate at finite isospin chemical potential μI. The phase diagram in the μI − μ plane is mapped out and shows a rich phase structure.nb_NO
dc.language.isoengnb_NO
dc.publisherAmerican Physical Societynb_NO
dc.titleChiral density wave versus pion condensation in the (1+1)-dimensional NJL modelnb_NO
dc.typeJournal articlenb_NO
dc.typePeer reviewednb_NO
dc.description.versionpublishedVersionnb_NO
dc.source.journalPhysical Review D. Particles and fieldsnb_NO
dc.identifier.doi10.1103/PhysRevD.95.054020
dc.identifier.cristin1461513
dc.description.localcode© 2017 American Physical Societynb_NO
cristin.unitcode194,66,20,0
cristin.unitnameInstitutt for fysikk
cristin.ispublishedtrue
cristin.fulltextpostprint
cristin.qualitycode0


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