A refined technique is described for approximating the numerically given radial part of atomic wave functions associated with self-consistent fields with exchange by means of Slater's analytical functions obtained by replacing each exponential in a hydrogen-like wave function by the sum of one, two, three, or more exponentials. Exponents and coefficients of these exponentials are calculated for the $3p$-function of Cl^-, corresponding to an accuracy of 0.0015 for the normalized radial part, and, with slightly less accuracy, for all the functions of two closed-shell ions, F^- (without exchange) and Na⁺, and for some neutral first-row atoms, C(¹D), N(²P), and O(¹S). The interpolation problem is discussed, and a new interpolation rule for the coefficients is stated, which gives excellent agreement (0.001) in the examples chosen, namely the $1s$-functions of the He-like ions and the $2p$-functions of Na⁺, Mg⁺², and Si⁺⁴.
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Per‐Olov Löwdin (1953) studied this question.
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