Parity Violating Bosonic Loops at Finite Temperature

Details Parity Violating Bosonic Loops at Finite Temperature Parity Violating Bosonic Loops at Finite Temperature

2001-10-17

arxiv.org/abs/hep-th/0110160v1

Phys.Rev.D65:085011,2002

Physics

High Energy Physics

High Energy Physics - Theory

10 pp, 1 fig, revtex

Scientific paper

10.1103/PhysRevD.65.085011

The finite temperature parity-violating contributions to the polarization tensor are computed at one loop in a system without fermions. The system studied is a Maxwell-Chern-Simons-Higgs system in the broken phase, for which the parity-violating terms are well known at zero temperature. At nonzero temperature the static and long-wavelength limits of the parity violating terms have very different structure, and involve non-analytic log terms depending on the various mass scales. At high temperature the boson loop contribution to the Chern-Simons term goes like T in the static limit and like T log T in the long-wavelength limit, in contrast to the fermion loop contribution which behaves like 1/T in the static limit and like log T/T in the long wavelength limit.

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