Excerpt from A Fortran Code for Calculation of Eigenvalues and Eigenfunctions in Real Potential Wells
Nuclear shell model calculations have until now employed almost exclusively harmonic oscillator wave functions for the evaluation of radial integrals. This has been done both for bound states and for states which actually belong to the continuum. The bound states evidently can be very well represented by harmonic oscillator wave functions. Any errors due to the difference between the actual optical potential and the har monic oscillator potential will in general be much smaller than the errors due to neglect of higher configurations. This is, however, not necessarily true for continuum states.
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