Phases of dense quarks at large

Abstract

Abstract In the limit of a large number of colors, N c , 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 ∼ N c 2 . When the quark chemical potential μ ∼ 1 , the deconfining transition temperature, T d , is independent of μ . For T T d , as μ increases above the mass threshold, baryons quickly form a dense phase where the pressure is ∼ N c . As illustrated by a Skyrme crystal, chiral symmetry can be both spontaneously broken, and then restored, in the dense phase. While the pressure is ∼ N c , 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.