A derivation and discussion of Armstrong's N-electron zero-momentum energy expression is presented. This functional Ezm(χ) is linear in the wave function χ, and thus is easier to compute and more sensitive to wave-function error than the variational upper bound Eᵥₐᵣ(χ). The smallness of the quantity Δ(χ)=Ezm(χ)-Eᵥₐᵣ(χ) provides an a priori criterion for assessment of the accuracy of an approximate wave function. Nontrivial numerical examples are given to illustrate the utility of this criterion.
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Thakkar et al. (1978) studied this question.
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