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Different forms of correlated atomic wavefunctions and their implications on the integrals occurring in calculations of variational solution to Schrödinger's equation are briefly discussed. A scheme for computing the integral ∫ f1(r1)f2(r2)f3(r3)g1(r12)g2(r23)g3(r31)(dv)is described and applied to the case gi(rij) = rijk.
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Öhrn et al. (1963) studied this question.
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