By means of a Langevin algorithm which incorporates the dynamical effects of various fermion species of nondegenerate masses, we simulate QCD with an isodoublet of quarks of mass 0.025 in lattice units and a heavier strange quark on an 8³×{}4 lattice. Our results suggest that the finite-temperature QCD phase transition in the real world is first order, that it is driven by the light condensate, and that it might be accompanied by a partial restoration of U(1)A symmetry.
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Gavai et al. (1988) studied this question.
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