Abstract

The operator S{\bf S} in Fock space which describes the scattering and particle production processes in an external time-dependent electromagnetic potential AA can be constructed from the one-particle S-matrix up to a physical phase λ[A]λ[A]. In this work we determine this phase for QEDQED in (2+1) dimensions, by means of causality, and show that no ultraviolet divergences arise, in contrast to the usual formalism of QEDQED.

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