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N-Electron Valence state Perturbation Theory
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 the quantum chemistry package DALTON.
The research performed into the development of this theory lead 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.
Additional recommended knowledge
Let be a zero-order CASCI wavefunction, defined as a linear combination of Slater determinants
obtained diagonalizing the true Hamiltonian inside the CASCI space
where 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 electrons are removed from the inactive part (core and virtual orbitals) and added to the valence part (active orbitals). At second order of perturbation . Decomposing the zero-order CASCI wavefunction as an antisymmetrized product of the inactive part Φc and a valence part
then the perturber wavefunctions can be written as
The pattern of inactive orbitals involved in the procedure can be grouped as a collective index l, so to represent the various perturber wavefunctions as , with μ an enumerator index for the different wavefunctions. The number of these functions is relative to the degree of contraction of the resulting perturbative space.
Supposing indexes i and j referring to core orbitals, a and b referring to active orbitals and r and s referring to virtual orbitals, the possible excitation schemes are:
These cases always represent situations where interclass electronic excitations happen. Other three excitation schemes involve a single interclass excitation plus an intraclass excitation internal to the active space:
Totally uncontracted approach
A possible approach is to define the perturber wavefunctions into Hilbert spaces defined by those determinants with given k and l labels. It is interesting to note that the determinants characterizing these spaces can be written as a partition comprising the same inactive (core + virtual) part and all possible valence (active) parts
The full dimensionality of these spaces can be exploited to obtain the definition of the perturbers, by diagonalizing the Hamiltonian inside them
This procedure is impractical given its high computational cost: for each space, a diagonalization of the true Hamiltonian must be performed. Computationally, is preferable to improve the theoretical development making use of the modified Dyall's Hamiltonian . This Hamiltonian behaves like the true Hamiltonian inside the CAS space, having the same eigenvalues and eigenvectors of the true Hamiltonian projected onto the CAS space. Also, given the decomposition for the wavefunction defined before, the action of the Dyall's Hamiltonian can be partitioned into
stripping out the constant contribution of the inactive part and leaving a subsystem to be solved for the valence part
The total energy is the sum of and the energies of the orbitals involved in the definition of the inactive part . This introduces the possibility to perform a single diagonalization of the valence Dyall's Hamiltonian on the CASCI zero-order wavefunction and evaluate the perturber energies using the property depicted above.
Strongly Contracted Approach
A different choice in the development of the NEVPT approach is to choose a single function for each space , leading to the Strongly Contracted (SC) scheme. A set of perturbative operators are used to produce a single function for each space, defined as the projection inside each space of the application of the Hamiltonian to the contracted zero order wavefunction. In other words
where is the projector onto the subspace. This can be equivalently written as the application of a specific part of the Hamiltonian to the zero-order wavefunction
For each space, appropriate operators can be devised. We will not present their definition, as it could result overkilling. Suffice to say that the resulting perturbers are not normalized, and their norm
plays an important role in the Strongly Contracted development. To evaluate these norms, the spinless density matrix of rank not higher than three between the functions are needed.
An important property of the is that any other function of the space which is orthogonal to do not interact with the zero-order wavefunction through the true Hamiltonian. It is possible to use the functions as a basis set for the expansion of the first-order correction to the wavefunction, and also for the expression of the zero-order Hamiltonian by means of a spectral decomposition
where are the normalized .
The expression for the first-order correction to the wavefunction is therefore
and for the energy is
It is important to note that this result still misses a definition of the perturber energies , which can be defined in a computationally advantageous approach by means of the Dyall's Hamiltonian
Developing the first term and extracting the inactive part of the Dyall's Hamiltonian it can be obtained
with Δεl equal to the sum of the orbital energies of the newly occupied virtual orbitals minus the orbital energies of the unoccupied core orbitals.
The term that still need to be evaluated is the braket involving the commutator. This can be obtained developing each V operator and substituting. To obtain the final result is necessary to evaluate Koopmans matrices and density matrices involving only active indexes. An interesting case is represented by the contribution for the case, which is trivial and can be demonstrated identical to the Møller-Plesset second-order contribution
NEVPT2 can therefore be seen as a generalized form of MP2 to multireference wavefunctions.
Partially Contracted Approach
An alternative approach, named Partially Contracted (PC) is to define the perturber wavefunctions in a subspace of with dimensionality higher than one (like in case of the Strongly Contracted approach). To define this subspace, a set of functions Φ is generated by means of the operators, after decontraction of their formulation. For example, in the case of the operator
The Partially Contracted approach makes use of functions and . These functions must be orthonormalized and purged of linear dependencies which may arise. The resulting set spans the space.
Once all the spaces have been defined, we can obtain as usual a set of perturbers from the diagonalization of the Hamiltonian (true or Dyall) inside this space
As usual, the evaluation of the Partially Contracted perturbative correction by means of the Dyall Hamiltonian involves simply manageable entities for nowadays computers.
Although the Strongly Contracted approach makes use of a perturbative space with very low flexibility, in general it provides values in very good agreement with those obtained by the more decontracted space defined for the Partially Contracted approach. This can be probably explained by the fact that the Strongly Contracted perturbers are a good average of the totally decontracted perturbative space.
It should also be noted that the Partially Contracted evaluation has a very little overhead in computational cost with respect to the Strongly Contracted one, therefore they are normally evaluated together.
NEVPT is blessed with many important properties, making the approach very solid and reliable. These properties arise both from the theoretical approach used and on the Dyall's Hamiltonian particular structure:
|This article is licensed under the GNU Free Documentation License. It uses material from the Wikipedia article "N-Electron_Valence_state_Perturbation_Theory". A list of authors is available in Wikipedia.|