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Epstein-Nesbet partitioning

As was shown by Claverie et al.46) this denominator shift leads to the same expression for k0 as does the Epstein-Nesbet partitioning of the Hamiltonian. [Pg.121]

Alternatively, excited state energies may be chosen to obtain a generalized Epstein-Nesbet (EN) partitioning... [Pg.261]

Double perturbation theory using Epstein-Nesbet partition. [Pg.228]

On the one hand, the Moller-Plesset partitioning of into and V is not unique and therefore the different orders of perturbation theory are also not uniquely defined. Various other choices of V were proposed " but they all led to different variants of the Epstein-Nesbet perturbation theory with a shifted denominator. This procedure also seems to be feasible for infinite systems, so there is hope that in the future more than 70 to 75% of the correlation energy will be obtained even in the second order. [Pg.197]

Table 1 Zero-order eigenvalues within the Epstein-Nesbet partitioning in multistate MCPT variants... Table 1 Zero-order eigenvalues within the Epstein-Nesbet partitioning in multistate MCPT variants...
Diagonal matrices E and E [ above contain zero-order energies corresponding to the model space and its complement, respectively. Zero-order energies in the Epstein-Nesbet (EN) partitioning [25, 26] are collected in Table 1 for completeness. [Pg.226]

Nakano, H. (1993a). MCSCF reference quasidegenerate perturbation theory with Epstein-Nesbet partitioning. The Journal of Chemical Physies, 99, 7983-7992. [Pg.629]

A related perturbation scheme is based on the Epstein-Nesbet partitioning of the Hamiltonian, where the zero-order operator contains those parts of the Hamiltonian that conserve the spin-orbital occupations... [Pg.217]

We note that this partitioning of the Hamiltonian eorresponds to that of Epstein-Nesbet theory the M0ller-Plesset partitioning has nonzero diagonal elements also in U. [Pg.248]

In addition to our earlier work (9,54), we wish to point out that we can also calculate the first-order coefficients by relying entirely on perturbation theory. Of course, the result will very much depend on the way we partition the Hamiltonian H into the unperturbed part Hq and the perturbation W, H -Hq+W. Since our zero-order wave function is assumed to represent a general multi-configurational Cl wave function, it is easier to employ the Epstein-Nesbet (EN) type perturbation theory. For this purpose we choose the unperturbed Hamiltonian Hq as follow... [Pg.20]

We advocate a particular choice of Hq which is akin to the Epstein-Nesbet (EN) partitioning for all the determinants which have at least... [Pg.119]


See other pages where Epstein-Nesbet partitioning is mentioned: [Pg.111]    [Pg.146]    [Pg.114]    [Pg.173]    [Pg.531]    [Pg.582]    [Pg.612]    [Pg.1056]    [Pg.275]    [Pg.122]    [Pg.96]    [Pg.100]    [Pg.320]   
See also in sourсe #XX -- [ Pg.96 ]




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