Viktor N.StaroverovEgorOspadov
Abstract
The exchange-correlation potential of the Kohn–Sham density-functional scheme is the difference between the Fermi potential—an effective potential appearing in the one-electron Schrödinger equation for the square root of the electron density—and the Pauli potential, i.e., vXC(r) = vF(r) − vP(r). We show that, for a given external potential and electron number, knowledge of vF(r) alone is sufficient to generate the corresponding vP(r) and vXC(r). The Fermi potential itself can be computed from the system's interacting two-electron reduced density matrix or modeled directly. The unified treatment of these three potentials provides a practical method for accessing accurate functional derivatives of the exchange-correlation, Pauli kinetic, and Levy–Perdew–Sahni energy functionals without having to tackle functional differentiation and numerical challenges of other construction techniques.
https://sci-hub.se/https://doi.org/10.1016/bs.aiq.2019.04.002
0 Comments