1977
DOI: 10.1103/physrevd.16.1169
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Fermions and gauge vector mesons at finite temperature and density. III. The ground-state energy of a relativistic quark gas

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Cited by 350 publications
(286 citation statements)
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“…As earlier, we ignore the normal state Hartree-Fock terms in the Schwinger-Dyson equation (49), and identify the thermodynamic potential in the normal phase with that of an ultrarelativistic, noninteracting Fermi gas of Fermi energy µ/3. We thus obtain [21] …”
Section: Ginzburg-landau Region At High Densitiesmentioning
confidence: 99%
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“…As earlier, we ignore the normal state Hartree-Fock terms in the Schwinger-Dyson equation (49), and identify the thermodynamic potential in the normal phase with that of an ultrarelativistic, noninteracting Fermi gas of Fermi energy µ/3. We thus obtain [21] …”
Section: Ginzburg-landau Region At High Densitiesmentioning
confidence: 99%
“…The first is the modification of the pairing interaction due to the pairing gap, which modifies the coefficients β 1 and β 2 of the fourth order terms in A. The second is radiative corrections by the normal medium [21] -i.e., quark self-energy, gluon polarization, and quark-quark-gluon and three-gluon vertex corrections -which modify the coefficients Eqs. (30)- (34), mainly through their dependence on N (µ/3) and T c .…”
Section: General Ginzburg-landau Approachmentioning
confidence: 99%
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“…They involve resumming the hard thermal loops (HTL), typically via the CornwallTouboulis-Jackiw two-particle irreducible (2PI) effective action [63], in which the complete propagator is used as an infinite set of variational parameters [64,65]. This has been used in approximately self-consistent HTL resummation calculations of the entropy by Blaizot, Iancu and Rebhan (BIR) [66] and of the pressure by Peshier [67].…”
Section: Equation Of Statementioning
confidence: 99%