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Fractional anomalous determinants and the chiral phase transition
high-energy-physics-latticehigh-energy-physics-phenomenologyhigh-energy-physics-theorynuclear-theorystrongly-correlated-electrons
At high temperature instantons form a dilute gas, so in QCD-like theories the breaking of the anomalous $U(1)_A$ symmetry is given by integral powers of the anomalous determinant, $\sim (\det Φ)^{Q}$, where $Φ\sim \overline{q}_L q_R$ is bilinear in the quark fields, and with untwisted boundary condi
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