Non-Perturbative QED and QCD at Finite Temperature

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dc.creatorStrickland, Michael
dc.date1998-09-30
dc.date.accessioned2026-07-07T04:05:15Z
dc.date.available2026-07-07T04:05:15Z
dc.descriptionWe present results of numerical solutions of Schwinger-Dyson equations for the finite-temperature quark and electron propagators. It is shown that both strongly coupled QED and QCD undergo a chiral symmetry restoring phase transition as the temperature is increased. We go beyond the bare vertex or "rainbow" approximation by applying the finite-temperature Ward-Takahashi identity to constrain the non-perturbative vertex function.
dc.descriptionTalk given at Fourth Workshop on Quantum Chromodynamics, 1-6 June 1998, The American University of Paris, Paris, France. 9 pages, 3 Postscript figures
dc.identifierhttps://arxiv.org/abs/hep-ph/9809592
dc.identifierhttp://arxiv.org/abs/hep-ph/9809592
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/48342
dc.subjectHigh Energy Physics - Phenomenology
dc.titleNon-Perturbative QED and QCD at Finite Temperature
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