The special case of three-dimensional quantum systems with a spherically symmetric interaction V(r) = V(r) permitting separation of the variables in the Schrödinger equation when it reduces to separate equations for the partial waves was already considered in Part I. There all attention was concentrated on the aspects of radial motion in a single independent channel.
KeywordsInverse Problem Schrodinger Equation Transverse Oscillation Closed Channel Channel Index
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