Physical Origin of the One-Quarter Exact Exchange in Density Functional Theory
Abstract
Exchange interactions are a manifestation of the quantum mechanical nature of the electrons and play a key role in predicting the properties of materials from first principles. In density functional theory (DFT), a widely used approximation to the exchange energy combines fractions of density-based and Hartree-Fock (exact) exchange. This so-called hybrid DFT scheme is accurate in many materials, for reasons that are not fully understood. Here we show that a 1/4 fraction of exact exchange plus a 3/4 fraction of density-based exchange is compatible with a correct quantum mechanical treatment of the exchange energy of an electron pair in the unpolarized electron gas. We also show that the 1/4 exact-exchange fraction mimics a correlation interaction between doubly-excited electronic configurations. The relation between our results and trends observed in hybrid DFT calculations is discussed, along with other implications.
Keywords
Cite
@article{arxiv.1810.02446,
title = {Physical Origin of the One-Quarter Exact Exchange in Density Functional Theory},
author = {Marco Bernardi},
journal= {arXiv preprint arXiv:1810.02446},
year = {2020}
}