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Gauge and global symmetries at high temperatureby: Steven Weinberg
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AbstractIt is shown how finite-temperature effects in a renormalizable quantum field theory can restore a symmetry which is broken at zero temperature. In general; for both gauge symmetries and ordinary symmetries; such effects occur only through a temperature-dependent change in the effective bare mass of the scalar bosons. The change in the boson bare mass is calculated for general field theories; and the results are used to derive the critical temperatures for a few special cases; including gauge and nongauge theories. In one case; it is found that a symmetry which is unbroken at low temperature can be broken by raising the temperature above a critical value. An appendix presents a general operator formalism for dealing with higher-order effects; and it is observed that the one-loop diagrams of field theory simply represent the contribution of zero-point energies to the free energy density. The cosmological implications of this work are briefly discussed.
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