Recently, we used Helmholtz's theorem to construct an unambiguous exchange᎐correlation energy density for use in density functional theory. This energy density requires only knowledge of the density dependence of the exchange᎐correlation energy functional, E , for its calculation. We calculate this
Virial exchange–correlation energy density in Hooke's atom
✍ Scribed by Kin-Chung Lam; Federico G. Cruz; Kieron Burke
- Publisher
- John Wiley and Sons
- Year
- 1998
- Tongue
- English
- Weight
- 211 KB
- Volume
- 69
- Category
- Article
- ISSN
- 0020-7608
No coin nor oath required. For personal study only.
✦ Synopsis
Application of the virial theorem to the interelectronic Coulomb repulsion
shows that the virial of the exchange potential yields the exchange energy. However, the virial of the correlation potential does not yield the correlation energy. We have recently constructed a ''hypercorrelated'' potential whose virial is the correlation energy. We apply these ideas to a system which contains two interacting electrons in an external harmonic potential, Hooke's atom. This system can be solved analytically for a set of spring constants and numerically for any spring constant. By inverting the Kohn᎐Sham equations, the exact exchange and correlation potentials can be found. These exact values are compared with several popular approximate functionals, namely local spin density Ž . Ž . Ž . LSD , Perdew, Burke, and Ernzerhof PBE , and Becke and Lee᎐Yang᎐Parr BLYP . We illustrate our results for two values of the spring constant. At a moderate value, the density is comparable to the He atom, while for a low spring constant, we explore extremely low densities.
📜 SIMILAR VOLUMES
Several different versions of density functional theory (DFT) that satisfy Hohenberg-Kohn theorems are characterized by different definitions of a reference or model state determined by an N-electron ground state. A common formalism is developed in which exact Kohn-Sham equations are derived for sta