Görling–Levy perturbation theory (GLPT) in Kohn–Sham (KS) density functional theory (DFT) is the analogue to what Møller–Plesset perturbation theory (MPPT) is in Hartree–Fock (HF) theory. Its basis is Rayleigh–Schrödinger perturbation theory (RSPT) and the adiabatic connection (AC). It describes electronic correlation effects. It is mostly used to second (GL2), rarely to third (GL3) or fourth (GL4) order, but becomes fast really increasingly computational expensive. It was published in 1993 and 1994 by Andreas Görling and Mel Levy.
Kohn–Sham correlation energy from Görling–Levy perturbation
The basis of GL perturbation theory is the adiabatic connection (AC) with the coupling constant 0 ≤ α ≤ 1 {\textstyle 0\leq \alpha \leq 1} connecting the artificial Kohn–Sham (KS) system of noninteracting electrons α = 0 {\textstyle \alpha =0} to the real system of interacting electrons α = 1 {\textstyle \alpha =1} with the AC Hamiltonian
H ^ α = T ^ + α V ^ ee + ∑ i = 1 N v α ( r i ) {\displaystyle {\hat {H}}_{\alpha }={\hat {T}}+\alpha {\hat {V}}_{\text{ee}}+\sum _{i=1}^{N}v_{\alpha }(r_{i})}
where N {\textstyle N} is the number of electrons, T ^ = − 1 2 ∑ i ∇ i 2 {\textstyle {\hat {T}}=-{\frac {1}{2}}\sum _{i}\nabla _{i}^{2}} the kinetic energy of the electrons, V ^ ee = ∑ i ∑ j > i | r i − r j | − 1 {\textstyle {\hat {V}}_{\text{ee}}=\sum _{i}\sum _{j>i}|r_{i}-r_{j}|^{-1}} the electron-electron interaction. Görling and Levy expressed the coupling-strength dependent local multiplicative potential under the constraint, that the density n ( r ) {\textstyle n(r)} stays fixed along the AC as
v α [ n ] ( r ) = v S [ n ] ( r ) − α v H x [ n ] ( r ) − v c α [ n ] ( r ) {\displaystyle v_{\alpha }[n](r)=v_{S}[n](r)-\alpha v_{Hx}[n](r)-v_{c}^{\alpha }[n](r)}
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