Abstract
We study symmetry and its relation to chiral symmetry at finite temperature through the application of functional renormalization group to the quark meson model. Very different from the mass gap and mixing angel between and mesons which are defined at mean field level and behavior like the chiral condensates, the topological susceptibility includes a fluctuations induced part which becomes dominant at high temperature. As a result, the symmetry is still considerably broken in the chiral symmetry restoration phase.
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