Condensates and pressure of two-flavor chiral perturbation theory at nonzero isospin and temperature
Abstract
We consider two-flavor chiral perturbation theory () at finite isospin chemical potential μI and finite temperature T. We calculate the effective potential and the quark and pion condensates as functions of T and μI to next-to-leading order in the low-energy expansion in the presence of a pionic source. We map out the phase diagram in the μI--T plane. Numerically, we find that the transition to the pion-condensed phase is second order in the region of validity of , which is in agreement with model calculations and lattice simulations. Finally, we calculate the pressure to two-loop order in the symmetric phase for nonzero μI and find that seems to be converging very well.
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