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Covariant calculations at finite temperature: The relativistic plasma

Journal Article · · Phys. Rev. D; (United States)

It is shown that finite-temperature calculations in field theory are manifestly Lorentz covariant at all stages if the Minkowski-space form of the temperature-dependent propagators is used and if the four-velocity u/sub ..mu../ of the heat bath is taken into account. New tensor structures involving u/sub ..mu../ generally arise but are severely constrained by covariant current conservation. A complete high-temperature (T>>m) expansion of the vacuum polarization tensor for non-Abelian gauge theories is computed to order g/sup 2/ and displays the separate dependence on frequency ..omega.. and wave number k that occurs at finite temperature. A covariant phenomenology of ''electric'' and ''magnetic'' properties is applied to the collective plasma effects, characterized by a plasma frequency ..omega../sub p/ /sup 2/ = (N/sub f/+2N)g/sup 2/T/sup 2//6 for SU(N) with N/sub f/ fermions. The longitudinal normal modes of the ''electric'' field exist only for ..omega..>..omega../sub p/; for ..omega..<..omega../sub p/ all ''electric'' fields are screened. The transverse normal modes are plane waves along E x B for ..omega..>..omega../sub p/; for ..omega..<..omega../sub p/ both transverse ''electric'' and ''magnetic'' fields are shielded except for the static (..omega.. = 0) case.

Research Organization:
Department of Physics, University of Pennsylvania, Philadelphia, Pennsylvania 19104
OSTI ID:
6702583
Journal Information:
Phys. Rev. D; (United States), Journal Name: Phys. Rev. D; (United States) Vol. 26:6; ISSN PRVDA
Country of Publication:
United States
Language:
English