On the use of resonant states in eigenfunction expansions of scattering and reaction amplitudes

Abstract The orthogonality and completeness properties of the resonant states as defined by Humblet and Rosenfeld are investigated using a simple regularization method first suggested by Zel'dovich. It is found that at leat for finite-range potentials, the set of bound states and any finite number of proper resonant states can be completed by a set of continuum states. This makes it possible to expand the scattering and reaction amplitudes in such a way that their resonance behabiour is exhibited, and the dependence of the corresponding partial widths on the interaction becomes more explicit.

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