Massless quantum electrodynamics with a critical point

dc.creatorBender, Carl M.
dc.creatorMilton, Kimball A.
dc.date1998-02-26
dc.date.accessioned2026-07-07T04:24:18Z
dc.date.available2026-07-07T04:24:18Z
dc.descriptionRecently, it has been observed that a quantum field theory need not be Hermitian to have a real, positive spectrum. What seems to be required is symmetry under combined parity and time-reversal transformations. This idea is extended to massless electrodynamics, in which the photon couples to the axial-vector current with an imaginary coupling constant. The eigenvalue condition necessary for the finiteness of the theory can now be solved; the value for the charge appears to be stable order-by-order. Similarly, the semiclassical Casimir model for the fine-structure constant yields a positive value.
dc.descriptionREVTeX, 6 pages, no figures
dc.identifierhttps://arxiv.org/abs/hep-th/9802184
dc.identifierhttp://arxiv.org/abs/hep-th/9802184
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/55362
dc.subjectHigh Energy Physics - Theory
dc.titleMassless quantum electrodynamics with a critical point
dc.typetext

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