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Multi configuration self-consistent field MCSCF

A configuration interaction calculation uses molecular orbitals that have been optimized typically with a Hartree-Fock (FIF) calculation. Generalized valence bond (GVB) and multi-configuration self-consistent field (MCSCF) calculations can also be used as a starting point for a configuration interaction calculation. [Pg.217]

The Multi-configuration Self-consistent Field (MCSCF) method can be considered as a Cl where not only the coefficients in front of the determinants are optimized by the variational principle, but also the MOs used for constructing the determinants are made optimum. The MCSCF optimization is iterative just like the SCF procedure (if the multi-configuration is only one, it is simply HF). Since the number of MCSCF iterations required for achieving convergence tends to increase with the number of configurations included, the size of MCSCF wave function that can be treated is somewhat smaller than for Cl methods. [Pg.117]

The Multi-Configuration Self-Consistent Field (MCSCF) method includes configurations created by excitations of electrons within an active space. Both the coefficients ca of the expansion in terms of CSFs and the expansion coefficients of the... [Pg.290]

By calculating A.U (R) and Al/ (i ) separately, we can straightforwardly calculate the total adiabatic correction V (R) for any isotopes of A and B. The adiabatic corrections are calculated by numerical differentiation of the multi-configurational self-consistent field (MCSCF) wave functions calculated with Dalton [23]. The nurnerical differentiation was performed with the Westa program developed 1986 by Agren, Flores-Riveros and Jensen [22],... [Pg.325]

Werner and co-workers [2, 21, 34] used internally-contracted multi-reference configuration-interaction (IC-MRCI) calculations, based on state-averaged (three-state) multi-configuration, self-consistent-field (MCSCF) calculations with large atomic orbital basis sets, to determine the three electronically adiabatic C1(F)+H2 PESs in the reactant arrangement L4, 2A, and lA. These all correlate with X( P) + H2. These three adiabatic electronic states are the IC-MRCI approximations to the three lowest eigenfunctions of Hgi, namely... [Pg.53]

For variational methods, such as Hartree-Fock (HF), multi-configurational self-consistent field (MCSCF), and Kohn-Sham density functional theory (KS-DFT), the initial values of the parameters are equal to zero and 0) thus corresponds to the reference state in the absence of the perturbation. The A operators are the non-redundant state-transfer or orbital-transfer operators, and carries no time-dependence (the sole time-dependence lies in the complex A parameters). Furthermore, the operator A (t)A is anti-Hermitian, and tlie exponential operator is thus explicitly unitary so that the norm of the reference state is preserved. Perturbation theory is invoked in order to solve for the time-dependence of the parameters, and we expand the parameters in orders of the perturbation... [Pg.44]

In the RISM-SCF procedure coupled with the multi-configurational self-consistent field (MCSCF) approach [59, 60, 61], the solvent effective potential modifying the electronic structure of the solute molecule is incorporated by adding a solvent term to the Fock operator of an... [Pg.251]

We will now briefly review some of the methods used to calculate the nonadiabatic coupling elements. As can be easily siumised, the computational scheme of nonadiabatic coupling elements depends heavily on the methods of electronic state calculation such as configuration interaction, multi configurational self consistent field (MCSCF) method, and so on. [Pg.258]

PHF methods can, in turn, be classified as the variational and nonvariational ones. In the former gronp of methods the coefficients in linear combination of Slater determinants and in some cases LCAO coefficients in HF MOs are optimized in the PHF calculations, in the latter such an optimization is absent. To the former group of PHF methods one refers different versions of the configuration interaction (Cl) method, the multi-configuration self-consistent field (MCSCF) method, the variational coupled cluster (CC) approach and the rarely used valence bond (VB) and generaUzed VB methods. The nonvariational PHF methods inclnde the majority of CC reaUza-tions and many-body perturbation theory (MBPT), called in its molecular realization the MoUer-Plessett (MP) method. In MP calculations not only RHF but UHF MOs are also used [107]. [Pg.150]

CASSCF is a variant of multi-configuration self-consistent field (MCSCF) theory. This means that in addition to the Cl expansion coefficients being varia-tionally optimized, the orbitals determining the expansion are also variationally optimized. Thus, the linear combination of atomic orbitals (LCAO) coefficients defining the orbitals is simultaneously optimized. If one starts with, for example, Hartree-Fock orbitals, then after the MCSCF wavefunction is optimized the orbitals will (often) be quite different. MCSCF wavefunctions thus contain the optimum orbitals for the given Cl expansion. CASSCF involves choosing a subset... [Pg.111]


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See also in sourсe #XX -- [ Pg.111 ]




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MCSCF

MCSCF (Multi-Configuration Self

MCSCF (multi-configurational self

MCSCF field

MCSCF self-consistent field

Multi configuration

Multi-Configuration Self Consistent Field

Multi-configuration self-consistent

Multi-configurational self consistent field

Multi-configurational self-consistent fields MCSCF)

Self multi-configuration

Self-Consistent Field

Self-consisting fields

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