We show that if one uses a screened Coulomb potential V(K)=4{π}/(K²+Kₛ²) to calculate γₓ, the exchange-energy density-functional gradient expansion coefficient, one obtains Sham's result if one takes K{→}0 before taking Kₛ{→}0. The exchange energy is by its very definition an unscreened quantity so that the correct order of the limits is Kₛ{→}0 before K{→}0, in which case γₓ=1.42γₓSham. .AE
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Kleinman et al. (1988) studied this question.
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