The infinite set of coupled equations in the adiabatic hyperspherical representation of two-electron correlated states is solved in the asymptotic region. The solution reveals that the longest-range couplings represent a partial transformation to independent-electron coordinates. Simple corrections to the phase shifts of H^- are obtained. Adiabatic and corrected phase shifts in the monopole approximation are compared with the Hartree-Fock phase shifts. Good agreement is obtained. The correction is applied to previously reported adiabatic phase shifts.
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J. H. Macek (1985) studied this question.
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