Please use this identifier to cite or link to this item: https://hdl.handle.net/2440/10935
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dc.contributor.authorBender, A.-
dc.contributor.authorPoulis, G.-
dc.contributor.authorRoberts, C.-
dc.contributor.authorSchmidt, S.-
dc.contributor.authorThomas, A.-
dc.date.issued1998-
dc.identifier.citationPhysics Letters B: Nuclear Physics and Particle Physics, 1998; 431(3-4):263-269-
dc.identifier.issn0370-2693-
dc.identifier.urihttp://hdl.handle.net/2440/10935-
dc.descriptionCopyright © 1998 Published by Elsevier Science B.V. All rights reserved-
dc.description.abstractIn a confining, renormalisable, Dyson-Schwinger equation model of two-flavour QCD we explore the chemical-potential dependence of the dressed-quark propagator, which provides a means of determining the behaviour of the chiral and deconfinement order parameters, and low-energy pion observables. We find coincident, first order deconfinement and chiral symmetry restoration transitions at μc = 375 MeV.fπ is insensitive to μ until μ ≈ μ0: = 0.7 μc when it begins to increase rapidly. mπ is weakly dependent on μ, decreasing slowly with μ and reaching a minimum 6% less than its μ = 0 value at μ = μ0. In a two-flavour free-quark gas at μ = μc the baryon number density would be approximately 3 ρ0, where ρ0 = 0.16 fm-3; while in such a gas at μ0 the density is ρ0. © 1998 Published by Elsevier Science B.V. All rights reserved.-
dc.description.statementofresponsibilityA. Bender, G. I. Poulis, C. D. Roberts, S. Schmidt and A. W. Thomas-
dc.language.isoen-
dc.publisherELSEVIER SCIENCE BV-
dc.source.urihttp://dx.doi.org/10.1016/s0370-2693(98)00546-2-
dc.titleDeconfinement at finite chemical potential-
dc.typeJournal article-
dc.identifier.doi10.1016/S0370-2693(98)00546-2-
pubs.publication-statusPublished-
dc.identifier.orcidThomas, A. [0000-0003-0026-499X]-
Appears in Collections:Aurora harvest 7
Special Research Centre for the Subatomic Structure of Matter publications

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