The Sternheimer quadrupole antishielding factor γ_∞ including self-consistency effects have been studied for several closed-shell ions isoelectronic with He, Ne, A, Kr, Xi, Cu⁺, and Ag⁺ in both free state as well as in ionic solid-state systems. Solid-state effects have been included using the Watson sphere model for ionic solids. The self-consistency contributions γ_∞⁽¹⁾ are found to be in general less than 30% of the zero-order antishielding factor γ_∞⁽⁰⁾. The net free ionic γ_∞(=γ_∞⁽⁰⁾+γ_∞⁽¹⁾) results agree very well with the results of corresponding coupled Hartree-Fock and polarized orbital calculations wherever available. For negative ions, γ_∞⁽⁰⁾ decreases significantly in going from the free ion to the solid state. For positive ions the opposite holds good. The solid-state effect on γ_∞⁽⁰⁾ is usually more important than the consistency effects γ_∞⁽¹⁾ for the negative ions. For positive ions, the two effects are comparable except in some cases where the consistency effects are larger in magnitude. These trends in the relative importance of γ_∞⁽¹⁾ as compared to solid-state effects are discussed in terms of the relative changes in the respective radial charge-density distributions in going from free ions to solid state. The possible influence of many-body correlations effects on γ_∞ is considered. Finally, the utility of the γ_∞ obtained in the present work for the net field gradients in ionic crystals, for which overlap and covalency effects between immediate neighbors have also to be considered, is discussed.
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Schmidt et al. (1980) studied this question.
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