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dc.contributor.authorAdhikari, Prabal
dc.contributor.authorAndersen, Jens Oluf
dc.contributor.authorKneschke, Patrick
dc.date.accessioned2017-12-19T14:58:49Z
dc.date.available2017-12-19T14:58:49Z
dc.date.created2017-02-26T21:34:38Z
dc.date.issued2017
dc.identifier.issn1550-7998
dc.identifier.urihttp://hdl.handle.net/11250/2473066
dc.description.abstractThe quark-meson model is often used as an effective low-energy model for QCD to study the chiral transition at finite temperature T and baryon chemical potential μB. The parameters in the quark-meson model can be found by expressing them in terms of the sigma mass mσ, the pion mass mπ, the constituent quark mass mq and the pion decay constant fπ. In practice, this matching is done at tree level, which is inconsistent once loop effects of the effective potential are taken into account. We show how to properly perform the matching in the quark-meson model by using the on-shell and the minimal subtraction renormalization schemes relating the physical masses and the pion decay constant to the running mass parameter and couplings. We map out the phase diagram in the μB–T plane and compare our results with other approximations.nb_NO
dc.language.isoengnb_NO
dc.publisherAmerican Physical Societynb_NO
dc.titleOn-shell parameter fixing in the quark-meson modelnb_NO
dc.typeJournal articlenb_NO
dc.typePeer reviewednb_NO
dc.description.versionpublishedVersionnb_NO
dc.source.volume95nb_NO
dc.source.journalPhysical Review Dnb_NO
dc.source.issue3nb_NO
dc.identifier.doi10.1103/PhysRevD.95.036017
dc.identifier.cristin1454035
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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