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Møller–Plesset perturbation theory : ウィキペディア英語版
Møller–Plesset perturbation theory

Møller–Plesset perturbation theory (MP) is one of several quantum chemistry post-Hartree–Fock ab initio methods in the field of computational chemistry. It improves on the Hartree–Fock method by adding electron correlation effects by means of Rayleigh–Schrödinger perturbation theory (RS-PT), usually to second (MP2), third (MP3) or fourth (MP4) order. Its main idea was published as early as 1934 by Christian Møller and Milton S. Plesset.〔

== Rayleigh–Schrödinger perturbation theory ==

The MP perturbation theory is a special case of RS perturbation theory. In RS theory one considers an unperturbed Hamiltonian operator \hat_, to which a small (often external) perturbation \hat is added:
:\hat = \hat_ + \lambda \hat.
Here, ''λ'' is an arbitrary real parameter that controls the size of the perturbation. In MP theory the zeroth-order wave function is an exact eigenfunction of the Fock operator, which thus serves as the unperturbed operator. The perturbation is the correlation potential.
In RS-PT the perturbed wave function and perturbed energy are expressed as a power series in λ:
: \Psi = \lim_ \sum_^ \lambda^ \Psi^,
: E = \lim_ \sum_^ \lambda^ E^.
Substitution of these series into the time-independent Schrödinger equation gives a new equation as m \to \infty:
: \left(\hat_ + \lambda V\right) \left(\sum_^m \lambda^ \Psi^\right) = \left(\sum_^m \lambda^ E^\right) \left(\sum_^m \lambda^ \Psi^\right).
Equating the factors of \lambda^k in this equation gives a ''k''th-order perturbation equation, where . See perturbation theory for more details.

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