Exact
density functionals for the exchange and correlation energies are
approximated in practical calculations for the ground-state electronic
structure of a many-electron system. An important exact constraint for
the construction of approximations is to recover the correct
non-relativistic large-Z expansions for the corresponding energies of neutral atoms with atomic number Z and electron number N = Z, which are correct to the leading order (−0.221Z5/3 and −0.021Z ln Z, respectively) even in the lowest-rung or local density approximation. We find that hydrogenic densities lead to Ex(N, Z) ≈ −0.354N2/3Z (as known before only for Z ≫ N ≫ 1) and Ec ≈ −0.02N ln N. These asymptotic estimates are most correct for atomic ions with large N and Z ≫ N, but we find that they are qualitatively and semi-quantitatively correct even for small N and N ≈ Z. The large-N asymptotic behavior of the energy is pre-figured in small-N
atoms and atomic ions, supporting the argument that widely predictive
approximate density functionals should be designed to recover the
correct asymptotics. It is shown that the exact Kohn–Sham correlation
energy, when calculated from the pure ground-state wavefunction, should
have no contribution proportional to Z in the Z → ∞ limit for any fixed N.
https://sci-hub.se/https://aip.scitation.org/doi/abs/10.1063/5.0017805?journalCode=jcp
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