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We consider a spin 1 2 electron in a translation-invariant model of non-relativistic Quantum Electrodynamics (QED). Let H(p, σ) denote the fiber Hamiltonian corresponding to the conserved momentum p ∈ R 3 , regu-larized by a fixed ultraviolet cutoff in its interaction term, and an infrared regularization parametrized by 0 < σ ≪ 1 which we ultimately remove(More)
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