Physics – High Energy Physics – High Energy Physics - Phenomenology
Scientific paper
1993-11-24
Phys.Rev.D49:3079-3082,1994
Physics
High Energy Physics
High Energy Physics - Phenomenology
7 pages + 2 figures, BNL-GGP-2
Scientific paper
10.1103/PhysRevD.49.R3079
As an extension of $QCD$, consider a theory with ``$2+1$'' flavors, where the current quark masses are held in a fixed ratio as the overall scale of the quark masses is varied. At nonzero temperature and baryon density it is expected that in the chiral limit the chiral phase transition is of first order. Increasing the quark mass from zero, the chiral transition becomes more weakly first order, and can end in a chiral critical point. We show that the only massless field at the chiral critical point is a sigma meson, with the universality class that of the Ising model. Present day lattice simulations indicate that $QCD$ is (relatively) near to the chiral critical point.
Gavin Sean
Gocksch Andreas
Pisarski Robert D.
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