Abstract
We present the “monomer dimer polymer MDP” representation of the partition function for strong coupling QCD with SU(2) gauge fields which is suitable for simulations at nonvanishing chemical potential μ (for the baryon number) and finite temperature T. We measured the chiral condensate, the baryonic number density and the Polyakov loop expectation value as function of T and μ. For large T or μ we observe a baryonic condensate and restoration of chiral symmetry.
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