Finite Temperature Effective Potential for Spontaneously Broken $λΦ^4$ Theory

dc.creatorNachbagauer, Herbert
dc.date1994-09-02
dc.date1994-09-03
dc.date.accessioned2026-07-07T09:00:03Z
dc.date.available2026-07-07T09:00:03Z
dc.descriptionWe present a self-consistent calculation of the finite temperature effective potential for $λΦ^4$ theory in four dimensions using a composite operator effective action. We find that in a spontaneously broken theory not only the so-called daisy and superdaisy graphs contribute to the next-to-leading order thermal mass, but also resummed non-local diagrams are of the same order, thus altering the effective potential at small effective mass.
dc.description5 pages, Talk held at the 'Workshop on Quantum Infrared Physics', 6-8 June at Paris
dc.identifierhttps://arxiv.org/abs/hep-ph/9409213
dc.identifierhttp://arxiv.org/abs/hep-ph/9409213
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/147928
dc.subjectHigh Energy Physics - Phenomenology
dc.titleFinite Temperature Effective Potential for Spontaneously Broken $λΦ^4$ Theory
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