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dc.contributor.authorAdhikari, Prabal
dc.contributor.authorAndersen, Jens Oluf
dc.contributor.authorKneschke, Patrick
dc.date.accessioned2019-03-13T09:28:19Z
dc.date.available2019-03-13T09:28:19Z
dc.date.created2018-10-18T16:30:07Z
dc.date.issued2018
dc.identifier.citationPhysical Review D. 2018, 98 (7), .nb_NO
dc.identifier.issn2470-0010
dc.identifier.urihttp://hdl.handle.net/11250/2589809
dc.description.abstractWe use the Polyakov-loop extended two-flavor quark-meson model as a low-energy effective model for QCD to study the phase diagram in the μI–T plane where μI is the isospin chemical potential. In particular, we focus on the Bose condensation of charged pions. At T=0, the onset of pion condensation is at μI=12mπ in accordance with exact results. The phase transition to a Bose-condensed phase is of second order for all values of μI and in the O(2) universality class. The chiral critical line joins the critical line for pion condensation at a point whose position depends on the Polyakov-loop potential and the sigma mass. For larger values of μI these curves are on top of each other. The deconfinement line enters smoothly the phase with the broken O(2) symmetry. We compare our results with recent lattice simulations and find overall good agreement.nb_NO
dc.language.isoengnb_NO
dc.publisherAmerican Physical Societynb_NO
dc.rightsNavngivelse 4.0 Internasjonal*
dc.rights.urihttp://creativecommons.org/licenses/by/4.0/deed.no*
dc.titlePion condensation and phase diagram in the Polyakov-loop quark-meson modelnb_NO
dc.typeJournal articlenb_NO
dc.typePeer reviewednb_NO
dc.description.versionpublishedVersionnb_NO
dc.source.pagenumber10nb_NO
dc.source.volume98nb_NO
dc.source.journalPhysical Review Dnb_NO
dc.source.issue7nb_NO
dc.identifier.doi10.1103/PhysRevD.98.074016
dc.identifier.cristin1621506
cristin.unitcode194,66,20,0
cristin.unitnameInstitutt for fysikk
cristin.ispublishedtrue
cristin.fulltextpostprint
cristin.qualitycode1


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