Alternatively, effective dynamic correlation can be introduced into the RAS-CI wave function by means of short-range density functional correlation energy. The idea relies on the different ability of wave function methods and DFT to treat non-dynamic and dynamic correlations. Concretely, the RAS-CI-srDFT (or RAS-srDFT) method136 is based on the range separation of the electron-electron Coulomb operator (ˆVee) through the error function to describe long-range interactions,
ˆVlr,μee=∑i<jerf(μrij)rij | (7.92) | ||
ˆVsr,μee=ˆVee-ˆVlr,μee | (7.93) |
where rij is the inter electronic distance and the parameter μ controls the extend of short- and long-range interactions. Such splitting of ˆVee provides a well-defined approach to merge WFT with DFT by applying ˆVlr,μee to RAS-CI and Vlr,μee to DFT. Within the RAS-srDFT approach, the energy of an electronic state can be expressed as:
ERAS-srDFT=minΨμ[⟨Ψμ|ˆT+ˆVne+ˆVlr,μee|Ψμ⟩+Esr,μH[ρ]+Esr,μxc[ρ]] | (7.94) |
where ρ≡ρ[Ψμ], and Esr,μH[ρ] and Esr,μxc[ρ] are the short-range Hartree and exchange-correlation energy functionals, respectively. The RAS-CI wave function can be combined with different short-range exchange and correlation functionals (Sections 5.3.2 and 5.3.3).