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Multi-reference Brillouin-Wigner perturbation

Multi-reference Brillouin-Wigner theory overcomes the intruder state problem because the exact energy is contained in the denominator factors. Calculations are therefore state specific , that is they are performed for one state at a time. This is in contrast to multi-reference Rayleigh-Schrddinger perturbation theory which is applied to a manifold of states simultaneously. Multi-reference Brillouin-Wigner perturbation theory is applied to a single state. Wenzel and Steiner [105] write (see also [106]) ... [Pg.41]

Whereas the multi-reference Rayleigh-Schrodinger perturbation theory approximates a manifold of states simultaneously, the multi-reference Brillouin-Wigner perturbation theory approach is applied to a single state - it is said to be state-specific . The multi-reference Brillouin-Wigner perturbation theory avoids the intruder state problem. If a particular Brillouin-Wigner-based formulation is not a valid many-body method, then a posteriori correction can be applied. This correction is designed to restore the extensivity of the method. This extensivity may be restored approximately... [Pg.31]

In this section we briefly survey the basic formalism of the multi-reference Brillouin-Wigner perturbation theory. This will serve to introduce our notation. [Pg.64]

It should be noted that the wave operator 17 no longer depends on the exact energies and therefore represents a much more suitable formulation for practical calculations. Within the multi-reference Brillouin-Wigner perturbation theory, we have been able to construct a multi-root wave operator together with an effective Hamiltonian operator, Jfeff, which formally possess the same properties as those employed in the multi-reference theories based on the Bloch equation. For this reason, the adjective multi-root is clearly not necessary here. [Pg.148]

Single-root formulation of multi-reference Brillouin-Wigner perturbation theory... [Pg.156]

In Section 4.2.3.2, we presented the basic equations of single-root (state-specific) multi-reference Brillouin-Wigner coupled cluster theory. We derived these equations from the single-root (state-specific) multi-reference Brillouin-Wigner perturbation theory presented in Section 4.2.3.1. In this section, we turn our attention to the coupled cluster single- and double-excitations approximation, ccsd. We present... [Pg.159]

Multi-reference Brillouin-Wigner perturbation theory for limited configuration interaction... [Pg.171]

We turn, in this section, to the multi-reference Brillouin-Wigner perturbation theory. We divide our discussion into two parts. In Section 4.4.2.1, we survey the basic theoretical apparatus of multi-reference second-order Brillouin-Wigner perturbation theory. In Section 4.4.3, we describe an a posteriori correction to multi-reference Brillouin-Wigner perturbation theory. [Pg.179]

If we restrict the order of perturbation admitted in (4.241) then we realize a finite order multi-reference Brillouin-Wigner perturbation theory. Specifically, if we neglect terms of order A are higher, we are led immediately to the second-order theory for which the matrix elements of the effective Hamiltonian (4.239) take the form ... [Pg.183]


See other pages where Multi-reference Brillouin-Wigner perturbation is mentioned: [Pg.42]    [Pg.52]    [Pg.28]    [Pg.156]    [Pg.156]    [Pg.171]    [Pg.178]    [Pg.193]    [Pg.196]   


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A posteriori correction to multi-reference Brillouin-Wigner perturbation theory

Brillouin-Wigner perturbation

Brillouin-Wigner perturbation theory multi-reference second order

Multi-reference Brillouin-Wigner perturbation theory

Multi-reference Brillouin-Wigner perturbation theory for limited configuration interaction

Multi-reference perturbation

Single-root formulation of multi-reference Brillouin-Wigner perturbation theory

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