Abstract
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 ${g}^{\ensuremath{-}1}$, in terms of the normal modes of the ${g}^{0}$ order Hamiltonian, taking into account the inelasticity caused by the existence of isobaric levels of the compound nucleon.
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