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The two-electron integrals which arise in electron-atomic ion scattering theory are expressed as a finite sum of terms each involving a generalized hypergeometric function. We give what is believed to be the first finite expansion known for the exchange integral. The many well-known recursive and transformation features of the hypergeometric functions are then utilized to conveniently and accurately evaluate the integrals with few restrictions on the values of the parameters.
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David E. Ramaker (1972) studied this question.
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