Coleman's theorem on physical assumptions for no Goldstone bosons in two dimensions

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dc.creatorItoi, Chigak
dc.date2003-03-13
dc.date2003-04-09
dc.date.accessioned2026-07-07T04:14:59Z
dc.date.available2026-07-07T04:14:59Z
dc.descriptionThirty years ago, Coleman proved that no continuous symmetry is broken spontaneously in a two-dimensional relativistic quantum field theory. In his argument, however, it is difficult to understand the physical meaning of the assumption of no infrared divergence. I derive the same result directly from the cluster property of a local field regarded as a physically acceptable assumption.
dc.description7 pages, no figures, corrected serious errors
dc.identifierhttps://arxiv.org/abs/hep-th/0303118
dc.identifierhttp://arxiv.org/abs/hep-th/0303118
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/51845
dc.subjectHigh Energy Physics - Theory
dc.subjectStatistical Mechanics
dc.subjectMathematical Physics
dc.titleColeman's theorem on physical assumptions for no Goldstone bosons in two dimensions
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