翻訳と辞書
Words near each other
・ "O" Is for Outlaw
・ "O"-Jung.Ban.Hap.
・ "Ode-to-Napoleon" hexachord
・ "Oh Yeah!" Live
・ "Our Contemporary" regional art exhibition (Leningrad, 1975)
・ "P" Is for Peril
・ "Pimpernel" Smith
・ "Polish death camp" controversy
・ "Pro knigi" ("About books")
・ "Prosopa" Greek Television Awards
・ "Pussy Cats" Starring the Walkmen
・ "Q" Is for Quarry
・ "R" Is for Ricochet
・ "R" The King (2016 film)
・ "Rags" Ragland
・ ! (album)
・ ! (disambiguation)
・ !!
・ !!!
・ !!! (album)
・ !!Destroy-Oh-Boy!!
・ !Action Pact!
・ !Arriba! La Pachanga
・ !Hero
・ !Hero (album)
・ !Kung language
・ !Oka Tokat
・ !PAUS3
・ !T.O.O.H.!
・ !Women Art Revolution


Dictionary Lists
翻訳と辞書 辞書検索 [ 開発暫定版 ]
スポンサード リンク

zero differential overlap : ウィキペディア英語版
zero differential overlap

Zero differential overlap is an approximation in computational molecular orbital theory that is the central technique of semi-empirical methods in quantum chemistry. When computers were first used to calculate bonding in molecules, it was possible to only calculate diatomic molecules. As computers advanced, it became possible to study larger molecules, but the use of this approximation has always allowed the study of even larger molecules. Currently semi-empirical methods can be applied to molecules as large as whole proteins. The approximation involves ignoring certain integrals, usually two-electron repulsion integrals. If the number of orbitals used in the calculation is N, the number of two-electron repulsion integrals scales as N4. After the approximation is applied the number of such integrals scales as N2, a much smaller number, simplifying the calculation.
==Details of approximation==
If the molecular orbitals \mathbf_i \ are expanded in terms of ''N'' basis functions, \mathbf_\mu^A \ as:-
:\mathbf_i \ = \sum_^N \mathbf_ \ \mathbf_\mu^A \,
where ''A'' is the atom the basis function is centred on, and \mathbf_ \ are coefficients, the two-electron repulsion integrals are then defined as:-
: \langle\mu\nu|\lambda\sigma\rangle = \iint \mathbf_\mu^A (1) \mathbf_\nu^B (1) \frac_\lambda^C (2) \mathbf_\sigma^D (2) d\tau_1\,d\tau_2 \
The zero differential overlap approximation ignores integrals that contain the product \mathbf_\mu^A (1) \mathbf_\nu^B (1) where ''μ'' is not equal to ''ν''. This leads to:-
: \langle\mu\nu|\lambda\sigma\rangle = \delta_ \delta_ \langle\mu\mu|\lambda\lambda\rangle
where \delta_ = \begin0 & \mu \ne \nu \\ 1 & \mu = \nu \ \end
The total number of such integrals is reduced to ''N''(''N'' + 1) / 2 (approximately ''N''2 / 2) from ()() / 2 (approximately ''N''4 / 8), all of which are included in ab initio Hartree–Fock and post-Hartree–Fock calculations.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
ウィキペディアで「zero differential overlap」の詳細全文を読む



スポンサード リンク
翻訳と辞書 : 翻訳のためのインターネットリソース

Copyright(C) kotoba.ne.jp 1997-2016. All Rights Reserved.