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图形展开函数方法中自旋轨道相互作用的评估。

Evaluation of the spin-orbit interaction within the graphically contracted function method.

机构信息

Chemical Sciences and Engineering Division, Argonne National Laboratory, Argonne, Illinois 60439, USA.

出版信息

J Phys Chem A. 2009 Nov 12;113(45):12741-7. doi: 10.1021/jp9059032.

Abstract

The graphically contracted function (GCF) method is extended to include an effective one-electron spin-orbit (SO) operator in the Hamiltonian matrix construction. Our initial implementation is based on a multiheaded Shavitt graph approach that allows for the efficient simultaneous computation of entire blocks of Hamiltonian matrix elements. Two algorithms are implemented. The SO-GCF method expands the spin-orbit wave function in the basis of GCFs and results in a Hamiltonian matrix of dimension N(dim)=N(alpha)((S(max) + 1)(2) - S(min)(2)). N(alpha) is the number of sets of nonlinear arc factor parameters, and S(min) and S(max) are respectively the minimum and maximum values of an allowed spin range in the wave function expansion. The SO-SCGCF (SO spin contracted GCF) method expands the wave function in a basis of spin contracted functions and results in a Hamiltonian matrix of dimension N(dim) = N(alpha). For a given N(alpha) and spin range, the number of parameters defining the wave function is the same in the two methods after accounting for normalization. The full Hamiltonian matrix construction with both approaches scales formally as O(N(alpha)(2)omegan(4)) for n molecular orbitals. The omega factor depends on the complexity of the Shavitt graph and includes factors such as the number of electrons, N, and the number of interacting spin states. Timings are given for Hamiltonian matrix construction for both algorithms for a range of wave functions with up to N = n = 128 and that correspond to an underlying linear full-CI CSF expansion dimension of over 10(75) CSFs, many orders of magnitude larger than can be considered using traditional CSF-based spin-orbit CI approaches. For Hamiltonian matrix construction, the SO-SCGCF method is slightly faster than the SO-GCF method for a given N(alpha) and spin range. The SO-GCF method may be more suitable for describing multiple states, whereas the SO-SCGCF method may be more suitable for describing single states.

摘要

图形收缩函数(GCF)方法扩展到哈密顿矩阵构建中,包括有效的单电子自旋轨道(SO)算符。我们的初始实现基于多头 Shavitt 图方法,允许高效地同时计算整个哈密顿矩阵元块。实现了两种算法。SO-GCF 方法在 GCF 基展开自旋轨道波函数,并导致维数为 N(dim)=N(alpha)((S(max) + 1)(2) - S(min)(2))的哈密顿矩阵。N(alpha)是非线性弧因子参数集的数量,S(min)和 S(max)分别是波函数展开中允许的自旋范围的最小值和最大值。SO-SCGCF(SO 自旋收缩 GCF)方法在自旋收缩函数的基展开波函数,并导致维数为 N(dim) = N(alpha)的哈密顿矩阵。对于给定的 N(alpha)和自旋范围,在考虑归一化后,两种方法定义波函数的参数数量相同。两种方法的全哈密顿矩阵构建形式上都以 O(N(alpha)(2)omegan(4))的比例缩放,其中 n 是分子轨道的数量,omega 因子取决于 Shavitt 图的复杂性,包括电子数 N 和相互作用自旋态的数量。对于多达 N = n = 128 的一系列波函数以及相应的基础线性完全 CI CSF 展开维数超过 10(75)CSFs 的情况,给出了两种算法的哈密顿矩阵构建的时间,这比使用传统基于 CSF 的自旋轨道 CI 方法可以考虑的大几个数量级。对于哈密顿矩阵构建,对于给定的 N(alpha)和自旋范围,SO-SCGCF 方法比 SO-GCF 方法稍快。SO-GCF 方法可能更适合描述多个态,而 SO-SCGCF 方法可能更适合描述单个态。

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