Abstract
A stationary Hilbert space scattering theory is derived for N‐body systems involving Coubomb‐like potentials. The derivation is based on stationary representations of the α‐channel renormalized wave operators, Ω(α)±, having the form Ω(α)±= s‐limε→+∞ W(α)±εP(α) F(α)±ε, where W(α)±εP(α) are the stationary operators which form the basis of short‐range stationary scattering theory and F(α)±ε* are appropriate stationary ’’renormalization’’ terms.

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