Near-locality of exchange and correlation density functionals for 1- and 2-electron systems
arXiv:1603.04062 · doi:10.1063/1.4950845
Abstract
The uniform electron gas and the hydrogen atom play fundamental roles in condensed matter physics and quantum chemistry. The former has an infinite number of electrons uniformly distributed over the neutralizing positively-charged background, and the latter only one electron bound to the proton. The uniform electron gas was used to derive the local spin density approximation (LSDA) to the exchange-correlation functional that undergirds the development of the Kohn-Sham density functional theory. We show here that the ground-state exchange-correlation energies of the hydrogen atom and many other 1- and 2-electron systems are modeled surprisingly well by a different local spin density approximation (LSDA0). Our LSDA0 is constructed to satisfy exact constraints, but agrees surprisingly well with the exact results for a uniform two-electron density in a finite, curved three-dimensional space. We also apply LSDA0 to excited or noded 1-electron densities. Furthermore, we show that the locality of an orbital can be measured by the ratio between the exact exchange energy and its optimal lower bound.
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- Local density approximations from finite systems
- Exchange functionals based on finite uniform electron gases
- Improving the applicability of the Pauli kinetic energy density based semilocal functional for solids
- Hartree potential dependent exchange functional
- How good are recent density functionals for ground and excited states of one-electron systems?
- A study of accurate exchange-correlation functionals through adiabatic connection
- A local tensor that unifies kinetic energy density and vorticity dependent exchange-correlation functionals
- Transient Uniform Electron Gases