The author is concerned with the calculation of the perturbed orbital wavefunction chosen to give the full polarizability of the ground and excited states of a complex atom. A new numerical technique is described and is tested on the hydrogen atom, where all polarized wavefunctions are analytic and known exactly. The accuracy obtained covers at least four significant places. Applications of these pseudo-states to the modified close coupling expansion are considered elsewhere.
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Vo Ky Lan (1972) studied this question.
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