Abstract

Statistical correlation coefficients τ[f] introduced by Kutzelnigg et al. [Phys. Rev. 172, 49 (1968)] provide overall measures of the difference between the electron-pair density and the product of single-electron densities, where f=f(r) is a probe function. It is shown that the angular correlation coefficient τ[r], a particular case of τ[f] for f(r)=r, is simply expressible in terms of the generalized electron-pair moments 〈q2〉(a,b) with two real-valued parameters a and b. Especially, the relation for a=b=1 means that τ[r] is nothing but the difference between the center-of-mass motion and relative motion contributions in the second electron-pair moments. Conversely, the electron-pair moments 〈q2〉(a,b) are obtained from the single-electron moment 〈∑iri2〉 and the correlation coefficient τ[r]. The same is also true in momentum space.

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