The optimized effective potential method (OEP) in Kohn-Sham (KS) density functional theory (DFT) is a method to determine the potentials as functional derivatives of the corresponding KS orbital-dependent energy density functionals. This can be in principle done for any arbitrary orbital-dependent functional, but is most common for exchange energy as the so-called exact exchange method (EXX), which will be considered here.
Origin The OEP method was developed more than 10 years prior to the work of Pierre Hohenberg, Walter Kohn and Lu Jeu Sham in 1953 by R. T. Sharp and G. K. Horton in order to investigate, what happens to Hartree-Fock (HF) theory when, instead of the regular nonlocal exchange potential, a local exchange potential is demanded. Much later after 1990 it was found out that this ansatz is useful in density functional theory.
Background via chain rule In density functional theory the exchange correlation (xc) potential is defined as the functional derivative of the exchange correlation (xc) energy with respect to the electron density ρ ( r ) {\displaystyle \rho (r)}
where the index s {\displaystyle s} denotes either occupied or unoccupied KS orbitals and eigenvalues. The problem is that, although the xc energy is in principle (due to the Hohenberg-Kohn (HK) theorem) a functional of the density, its explicit dependence on the density is unknown (only known in the simple Local density approximation (LDA) case), only its implicit dependence through the KS orbitals. That motivates the use of the chain rule
v x c ( r ) = ∫ d r ′ ∑ s [ δ E x c [ { ϕ s } ] δ ϕ s ( r ′ ) δ ϕ s ( r ′ ) δ ρ ( r ) + c . c . ] {\displaystyle v_{xc}(r)=\int dr'\sum _{s}{\bigg [}{\frac {\delta E_{xc}[\{\phi _{s}\}]}{\delta \phi _{s}(r')}}{\frac {\delta \phi _{s}(r')}{\delta \rho (r)}}+c.c.{\bigg ]}}
Unfortunately the functional derivative δ ϕ s / δ ρ {\displaystyle \delta \phi _{s}/\delta \rho } , despite its existence, is also unknown. So one needs to invoke the chain rule once more, now with respect to the Kohn-Sham (KS) potential v S ( r ) {\displaystyle v_{S}(r)}
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