Lattice QCD at finite isospin density at zero and finite temperature
arXiv:hep-lat/0202028 · doi:10.1103/PhysRevD.66.034505
Abstract
We simulate lattice QCD with dynamical and quarks at finite chemical potential, , for the third component of isospin (), at both zero and at finite temperature. At zero temperature there is some , say, above which and parity are spontaneously broken by a charged pion condensate. This is in qualitative agreement with the prediction of effective (chiral) Lagrangians which also predict . This transition appears to be second order, with scaling properties consistent with the mean-field predictions of such effective Lagrangian models. We have also studied the restoration of symmetry at high temperature for . For sufficiently large, this finite temperature phase transition appears to be first order. As is decreased it becomes second order connecting continuously with the zero temperature transition.
23 pages, Revtex, 9 figures. Major revision of sections 3 and 4 to include new analyses of critical scaling which we now find to be in the universality class of mean-field theory
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