Chiral phase transition in a covariant nonlocal NJL model

The properties of the chiral phase transition at finite temperature and chemical potential are investigated within a nonlocal covariant extension of the Nambu-Jona-Lasinio model based on a separable quark-quark interaction. We consider both the situation in which the Minkowski quark propagator has p...

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Bibliographic Details
Authors: General, Ignacio; Gomez Dumm, Daniel Alberto; Scoccola, Norberto Nerio
Format: Article
Status:Published version
Publication date:2001
Country:Argentina
Institution:Consejo Nacional de Investigaciones Científicas y Técnicas
Repository:CONICET Digital (CONICET)
Language:English
OAI Identifier:oai:ri.conicet.gov.ar:11336/71720
Online Access:http://hdl.handle.net/11336/71720
Access Level:Open access
Keyword:CHIRAL PHASE TRANSITION
FINITE TEMPERATURE AND/OR DENSITY
NONLOCAL NAMBU-JONA-LASINIO MODEL
https://purl.org/becyt/ford/1.3
https://purl.org/becyt/ford/1
Description
Summary:The properties of the chiral phase transition at finite temperature and chemical potential are investigated within a nonlocal covariant extension of the Nambu-Jona-Lasinio model based on a separable quark-quark interaction. We consider both the situation in which the Minkowski quark propagator has poles at real energies and the case where only complex poles appear. In the literature, the latter has been proposed as a realization of confinement. In both cases, the behaviour of the physical quantities as functions of T and μis found to be quite similar. In particular, for low values of T the chiral transition is always of first order and, for finite quark masses, at certain "end point" the transition turns into a smooth crossover. In the chiral limit, this "end point" becomes a "tricritical" point. Our predictions for the position of these points are similar, although somewhat smaller, than previous estimates. Finally, the relation between the deconfining transition and chiral restoration is also discussed.