Extension of the Nambu--Jona-Lasinio model at high densities and temperatures by using an implicit regularization scheme

Details Extension of the Nambu--Jona-Lasinio model at high densities and temperatures by using an implicit regularization scheme Extension of the Nambu--Jona-Lasinio model at high densities and temperatures by using an implicit regularization scheme

2006-04-24

arxiv.org/abs/hep-ph/0604203v3

Phys.Rev.C77:065201,2008

Physics

High Energy Physics

High Energy Physics - Phenomenology

7 pages, 5 eps figures - in version 3, substantial changes in text, results and conclusions unchanged. To be published in Phys

Scientific paper

10.1103/PhysRevC.77.065201

Traditional cutoff regularization schemes of the Nambu--Jona-Lasinio model limit the applicability of the model to energy-momentum scales much below the value of the regularizing cutoff. In particular, the model cannot be used to study quark matter with Fermi momenta larger than the cutoff. In the present work an extension of the model to high temperatures and densities recently proposed by Casalbuoni, Gatto, Nardulli, and Ruggieri is used in connection with an implicit regularization scheme. This is done by making use of scaling relations of the divergent one-loop integrals that relate these integrals at different energy-momentum scales. Fixing the pion decay constant at the chiral symmetry breaking scale in the vacuum, the scaling relations predict a running coupling constant that decreases as the regularization scale increases, implementing in a schematic way the property of asymptotic freedom of quantum chromodynamics. If the regularization scale is allowed to increase with density and temperature, the coupling will decrease with density and temperature, extending in this way the applicability of the model to high densities and temperatures. These results are obtained without specifying an explicit regularization. As an illustration of the formalism, numerical results are obtained for the finite density and finite temperature quark condensate, and to the problem of color superconductivity at high quark densities and finite temperature.

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