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dc.contributor.authorAdhikari, Prabal
dc.contributor.authorAndersen, Jens Oluf
dc.contributor.authorKneschke, Patrick
dc.date.accessioned2018-03-23T12:48:41Z
dc.date.available2018-03-23T12:48:41Z
dc.date.created2017-07-24T20:26:07Z
dc.date.issued2017
dc.identifier.citationPhysical Review D. 2017, 96 (1).nb_NO
dc.identifier.issn2470-0010
dc.identifier.urihttp://hdl.handle.net/11250/2491944
dc.description.abstractThe two-flavor quark-meson model is used as a low-energy effective model for QCD to study inhomogeneous chiral condensates at finite baryon chemical potential μB . The parameters of the model are determined by matching the meson and quark masses, and the pion decay constant to their physical values using the on-shell and modified minimal subtraction schemes. Using a chiral-density wave ansatz for the inhomogeneity, we calculate the effective potential in the mean-field approximation and the result is completely analytic. The size of the inhomogeneous phase depends sensitively on the pion mass and whether one includes the vacuum fluctuations or not. Finally, we briefly discuss the mean-field phase diagram.© 2017 American Physical Societynb_NO
dc.language.isoengnb_NO
dc.publisherAmerican Physical Societynb_NO
dc.titleInhomogeneous chiral condensate in the quark-meson modelnb_NO
dc.typeJournal articlenb_NO
dc.typePeer reviewednb_NO
dc.description.versionpublishedVersionnb_NO
dc.source.pagenumber14nb_NO
dc.source.volume96nb_NO
dc.source.journalPhysical Review Dnb_NO
dc.source.issue1nb_NO
dc.identifier.doi10.1103/PhysRevD.96.016013
dc.identifier.cristin1482999
dc.description.localcode© 2017 American Physical Societynb_NO
cristin.unitcode194,66,20,0
cristin.unitnameInstitutt for fysikk
cristin.ispublishedtrue
cristin.fulltextpostprint
cristin.fulltextoriginal
cristin.qualitycode1


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