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Phases of dense quarks at large

2007/06/30 by Larry McLerran, Robert D. Pisarski · 744 citations
Physics and Astronomy · #Baryon #Condensed matter physics #Gluon #Hadron #High-Energy Particle Collisions Research #Particle physics #Particle physics theoretical and experimental studies #Phase (matter) #Phase diagram #Phase transition #Physics #Quantum Chromodynamics and Particle Interactions #Quantum chromodynamics #Quantum mechanics #Quark #Quark–gluon plasma #hep-ph

paper · pdf · doi:10.1016/j.nuclphysa.2007.08.013

published in Nuclear Physics A 796(1-4), 83-100 (Elsevier BV) · 23 pages, 2 figures, uses entcs macro. Minor changes in wording

arxiv created 2007/08/10 · openalex publication_date 2007/09/15 · arxiv updated 2010/04/06 · openalex created_date 2016/06/24 · openalex updated_date 2026/08/05

Abstract

In the limit of a large number of colors, Nc, we suggest that gauge theories can exhibit several distinct phases at nonzero temperature and quark density. Two are familiar: a cold, dilute phase of confined hadrons, where the pressure is ~ 1, and a hot phase of deconfined quarks and gluons, with pressure ~ Nc2. When the quark chemical potential mu ~ 1, the deconfining transition temperature, Td, is independent of mu. For T < Td, as mu increases above the mass threshold, baryons quickly form a dense phase where the pressure is ~ Nc. As illustrated by a Skyrme crystal, chiral symmetry can be both spontaneously broken, and then restored, in the dense phase. While the pressure is ~ Nc, like that of (non-ideal) quarks, the dense phase is still confined, with interactions near the Fermi surface those of baryons, and not of quarks. Thus in the chirally symmetric region, baryons near the Fermi surface are parity doubled. We suggest possible implications for the phase diagram of QCD.

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