dc.contributorUniversidade Estadual Paulista (Unesp)
dc.contributorUniv Tecnol Fed Parana
dc.contributorUniversidade Federal do ABC (UFABC)
dc.date.accessioned2014-12-03T13:11:19Z
dc.date.available2014-12-03T13:11:19Z
dc.date.created2014-12-03T13:11:19Z
dc.date.issued2014-01-20
dc.identifierPhysics Letters B. Amsterdam: Elsevier Science Bv, v. 728, p. 626-629, 2014.
dc.identifier0370-2693
dc.identifierhttp://hdl.handle.net/11449/113007
dc.identifier10.1016/j.physletb.2013.12.042
dc.identifierWOS:000330556000094
dc.identifierWOS000330556000094.pdf
dc.description.abstractThe chiral symmetry breaking transition of quarks in the fundamental and adjoint representation is studied in a model where the gap equation contains two contributions, one containing a confining propagator and another corresponding to the exchange of one-dressed dynamically massive gluons. When quarks are in the fundamental representation the confinement effect dominates the chiral symmetry breaking while the gluon exchange is suppressed due to the dynamical gluon mass effect in the propagator and in the coupling constant. In this case the chiral and deconfinement transition temperatures are approximately the same. For quarks in the adjoint representation, due to the larger Casimir eigenvalue, the gluon exchange is operative and the chiral transition happens at a larger temperature than the deconfinement one. (C) 2013 The Authors. Published by Elsevier B.V. All rights reserved.
dc.languageeng
dc.publisherElsevier B.V.
dc.relationPhysics Letters B
dc.relation4.254
dc.relation2,336
dc.rightsAcesso aberto
dc.sourceWeb of Science
dc.subjectGeneral properties of QCD
dc.subjectLattice QCD calculations
dc.subjectOther nonperturbative calculations
dc.titleChiral transition of fundamental and adjoint quarks
dc.typeArtículos de revistas


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