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We calculate binding energies for heliumlike ions of variable dimensionality (D) with the wave functions A=e^(-αR₁-βR₂)+e^(-βR₁-αR₂) and B=A(1+cR₁₂). The binding energy decreases with increasing D. Functions A and B predict "critical binding dimensionalities" at D=3.99 and 4.89, respectively, above which there is no binding in the hydride anion. The exact ground-state binding energy at $D=5$ is shown to be equal to that of the doubly excited 2p² ³Pᵉ state into in three dimensions. By "dimensionality scaling" of atomic units the $D=1$ atom is transformed the δ-function model for which exact energies are known. In the infinite dimensional limit, function A predicts no exchange contribution to binding for nuclear charge Z≥2, with α≠β only for Z<2.
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Herrick et al. (1975) studied this question.
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