The strong coupling theory of meson scattering by nucleons is extended to second order in the inverse of the coupling parameter g for the case of a charged scalar field. The ordinary and charge exchange scattering amplitudes for positive and negative mesons are calculated by a perturbation expansion in g^-1, in terms of the normal modes of the g⁰ order Hamiltonian, taking into account the inelasticity caused by the existence of isobaric levels of the compound nucleon.
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Allan N. Kaufman (1953) studied this question.
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