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An expansion of the three-body Coulomb potential in generalized angular-momentum eigenfunctions developed earlier by one of the authors is used to compute energy eigenvalues and eigenfunctions of bound S states of three-body Coulomb systems. The results for He, H^-, e^-e⁺e^-, and pμ^-p are compared with the results of other computational approaches.
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Whitten et al. (1974) studied this question.
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