Abstract

We consider a charged particle, spin 1 2 , with relativistic kinetic energy and minimally coupled to the quantized Maxwell field. Since the total momentum is conserved, the Hamiltonian admits a fiber decomposition as H ( P ) , P ∈ R 3 . We study the spectrum of H ( P ) . In particular we prove that, for non-zero photon mass, the ground state is exactly two-fold degenerate and separated by a gap, uniformly in P, from the rest of the spectrum.

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