Parity Violating Bosonic Loops at Finite Temperature

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dc.creatorAlves, V. S.
dc.creatorDas, Ashok
dc.creatorDunne, Gerald V.
dc.creatorPerez, Silvana
dc.date2001-10-17
dc.date.accessioned2026-07-07T11:31:56Z
dc.date.available2026-07-07T11:31:56Z
dc.descriptionThe 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.
dc.description10 pp, 1 fig, revtex
dc.identifierhttps://arxiv.org/abs/hep-th/0110160
dc.identifierhttp://arxiv.org/abs/hep-th/0110160
dc.identifierPhys.Rev.D65:085011,2002
dc.identifierdoi:10.1103/PhysRevD.65.085011
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/197435
dc.subjectHigh Energy Physics - Theory
dc.subjectHigh Energy Physics - Phenomenology
dc.titleParity Violating Bosonic Loops at Finite Temperature
dc.typetext

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