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“N 个电子在 M 轨道”的活性空间的自旋耦合理论。

Spin-coupled theory for 'N electrons in M orbitals' active spaces.

机构信息

Department of Chemistry, University of York, Heslington, York, YO10 5DD, United Kingdom.

出版信息

J Phys Chem A. 2012 Jul 5;116(26):7238-44. doi: 10.1021/jp303998h. Epub 2012 Jun 22.

DOI:10.1021/jp303998h
PMID:22690866
Abstract

Spin-coupled (SC) theory, an ab initio valence bond (VB) approach which uses a compact and an easy-to-interpret single-orbital product wave function comparable in quality to a ‘N in N’ complete-active-space self-consistent field [CASSCF(N,N)] construction, is extended to ‘N in M’ (N ≠ M) active spaces. The SC(N,M) wave function retains the essential features of the original SC model: It involves just the products of nonorthogonal orbitals covering all distributions of N electrons between M orbitals in which as few orbitals as possible, |N – M|, are doubly occupied (for N > M) or missing (for N < M) and all other orbitals are singly occupied; each of these products is combined with a flexible spin function which allows any mode of coupling of the spins of the orbitals within the product. The SC(N,M) wave function remains much more compact than a CASSCF(N,M) construction; for example, the SC(6,7) wave function includes 35 configuration state functions (CSFs) as opposed to the 490 CSFs in the CASSCF case. The essential features of the SC(N,M) method are illustrated through a SC(6,5) calculation on the cyclopentadienyl anion, C5H5(–), and a SC(6,7) calculation on the tropylium cation, C7H7(+). The SC(6,5) and SC(6,7) wave functions for C5H5(–) and C7H7(+) are shown to provide remarkably clear modern VB models for the electronic structures of these aromatic cyclic ions which closely resemble the well-known SC model of benzene and yet recover almost all of the correlation energy included in the corresponding CASSCF(6,5) and CASSCF(6,7) wave functions: over 97% in the case of C5H5(–) and over 95% in the case of C7H7(+).

摘要

自旋耦合(SC)理论是一种从头算价键(VB)方法,它使用一种紧凑且易于解释的单轨道乘积波函数,其质量可与“N in N”完全活性空间自洽场[CASSCF(N,N)]构造相媲美,该方法被扩展到“N in M”(N ≠ M)活性空间。SC(N,M)波函数保留了原始 SC 模型的基本特征:它仅涉及覆盖 M 轨道中 N 个电子的所有分布的非正交轨道的乘积,其中尽可能少的轨道|N – M|被双占据(对于 N > M)或缺失(对于 N < M),并且所有其他轨道都被单占据;这些乘积中的每一个都与一个灵活的自旋函数相结合,该函数允许轨道内的自旋以任何方式耦合。与 CASSCF(N,M)构造相比,SC(N,M)波函数仍然要紧凑得多;例如,SC(6,7)波函数包括 35 个组态态函数(CSF),而 CASSCF 情况下则有 490 个 CSF。通过对环戊二烯阴离子 C5H5(–)的 SC(6,5)计算和对 tropylium 阳离子 C7H7(+)的 SC(6,7)计算,说明了 SC(6,5)和 SC(6,7)方法的基本特征。SC(6,5)和 SC(6,7)波函数为 C5H5(–)和 C7H7(+)提供了非常清晰的现代 VB 模型,这些模型与著名的苯 SC 模型非常相似,但几乎恢复了包含在相应 CASSCF(6,5)和 CASSCF(6,7)波函数中的所有相关能量:在 C5H5(–)的情况下超过 97%,在 C7H7(+)的情况下超过 95%。

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