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We calculate the Hohenberg-Kohn-Sham energy response kernel Kxc(q) exactly for the high-density electron gas, and thus generalize the classic work of Ma and Brueckner to finite wave vector. The results are relevant to (1) density-functional theory, where we verify that one of the key assumptions used in the Langreth-Mehl functional was qualitatively correct and suggest possible improvements; (2) dielectric response theory, where we exactly calculate the leading correction to the static Lindhard screening function; and (3) a static attractive 1/r⁶-like interaction between like-charged point particles---we verify the recent suggestion of Maggs and Ashcroft that such an interaction exists and calculate its value.
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Langreth et al. (1987) studied this question.
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