Abstract:
We investigate the p-state mean-field model of the Potts glass
for 2 < p < 4 below the continuous phase transition to the glassy
phase. It is generally believed that the first replica
symmetry breaking solution describes the low temperature
equilibrium state. We find out apart from a solution with the
first hierarchical level of replica-symmetry breaking, which is
locally stable close to the transition point, another
hierarchical solution that in the limit of the infinitely
breaking symmetry scheme agrees with the continuous full
replica-symmetry breaking solution (FRSB). The latter is
marginally stable and has higher free energy than the former.
We argue that the true equilibrium is reached only by FRSB
being globally stable.