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Lattice QCD at finite isospin density at zero and finite temperature

J. B. Kogut

D. K. Sinclair

  • Department of Physics, University of Illinois, 1110 West Green Street, Urbana, Illinois 61801-3080

  • HEP Division, Argonne National Laboratory, 9700 South Cass Avenue, Argonne, Illinois 60439

Phys. Rev. D 66, 034505 – Published 22 August, 2002

DOI: https://doi.org/10.1103/PhysRevD.66.034505

Abstract

We simulate lattice QCD with dynamical u and d quarks at finite chemical potential, μI, for the third component of isospin (I3) at both zero and at finite temperature. At zero temperature there is some μI, μc say, above which I3 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 μc=mπ. 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 I3 symmetry at high temperature for μI>μc. For μI sufficiently large, this finite temperature phase transition is very abrupt, suggesting that it is first order. As μI is decreased it appears to become second order connecting continuously with the zero temperature transition.

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