In quantum chemistry, n-electron valence state perturbation theory (NEVPT) is a perturbative treatment applicable to multireference CASCI-type wavefunctions. It can be considered as a generalization of the well-known second-order Møller–Plesset perturbation theory to multireference complete active space cases. The theory is directly integrated into many quantum chemistry packages such as MOLCAS, Molpro, DALTON, PySCF and ORCA. The research performed into the development of this theory led to various implementations. The theory here presented refers to the deployment for the single-state NEVPT, where the perturbative correction is applied to a single electronic state. Research implementations has been also developed for quasi-degenerate cases, where a set of electronic states undergo the perturbative correction at the same time, allowing interaction among themselves. The theory development makes use of the quasi-degenerate formalism by Lindgren and the Hamiltonian multipartitioning technique from Zaitsevskii and Malrieu.
Theory Let Ψ m ( 0 ) {\displaystyle \Psi _{m}^{(0)}} be a zero-order CASCI wavefunction, defined as a linear combination of Slater determinants
Ψ m ( 0 ) = ∑ I ∈ C A S C I , m | I ⟩ {\displaystyle \Psi _{m}^{(0)}=\sum _{I\in {\rm {CAS}}}C_{I,m}\left|I\right\rangle }
obtained diagonalizing the true Hamiltonian H ^ {\displaystyle {\hat {\mathcal {H}}}} inside the CASCI space
P ^ C A S H ^ P ^ C A S | Ψ m ( 0 ) ⟩ = E m ( 0 ) | Ψ m ( 0 ) ⟩ {\displaystyle {\hat {\mathcal {P}}}_{\rm {CAS}}{\hat {\mathcal {H}}}{\hat {\mathcal {P}}}_{\rm {CAS}}\left|\Psi _{m}^{(0)}\right\rangle =E_{m}^{(0)}\left|\Psi _{m}^{(0)}\right\rangle }
where P ^ C A S {\displaystyle {\hat {\mathcal {P}}}_{\rm {CAS}}} is the projector inside the CASCI space. It is possible to define perturber wavefunctions in NEVPT as zero-order wavefunctions of the outer space (external to CAS) where k {\displaystyle k} electrons are removed from the inactive part (core and virtual orbitals) and added to the valence part (active orbitals). At second order of perturbation − 2 ≤ k ≤ 2 {\displaystyle -2\leq k\leq 2} . Decomposing the zero-order CASCI wavefunction as an antisymmetrized product of the inactive part Φ c {\displaystyle \Phi _{c}} and a valence part Ψ m v {\displaystyle \Psi _{m}^{v}}
| Ψ m ( 0 ) ⟩ = | Φ c Ψ m v ⟩ {\displaystyle \left|\Psi _{m}^{(0)}\right\rangle =\left|\Phi _{c}\Psi _{m}^{v}\right\rangle }
then the perturber wavefunctions can be written as
| Ψ l , μ k ⟩ = | Φ l − k Ψ μ v + k ⟩ {\displaystyle \left|\Psi _{l,\mu }^{k}\right\rangle =\left|\Phi _{l}^{-k}\Psi _{\mu }^{v+k}\right\rangle }
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