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包含三重激发的耦合簇方法用于自由基激发态的研究。

Coupled cluster methods including triple excitations for excited states of radicals.

作者信息

Smith Christopher E, King Rollin A, Crawford T Daniel

机构信息

Department of Chemistry, Virginia Tech, Blacksburg, VA 24061, USA.

出版信息

J Chem Phys. 2005 Feb 1;122(5):54110. doi: 10.1063/1.1835953.

DOI:10.1063/1.1835953
PMID:15740313
Abstract

We report an extension of the coupled cluster iterative-triples model, CC3, to excited states of open-shell molecules, including radicals. We define the method for both spin-unrestricted Hartree-Fock (UHF) and spin-restricted open-shell Hartree-Fock (ROHF) reference determinants and discuss its efficient implementation in the PSI3 program package. The program is streamlined to use at most O(N(7)) computational steps and avoids storage of the triple-excitation amplitudes for both the ground- and excited-state calculations. The excitation-energy program makes use of a Lowdin projection formalism (comparable to that of earlier implementations) that allows computational reduction of the Davidson algorithm to only the single- and double-excitation space, but limits the calculation to only one excited state at a time. However, a root-following algorithm may be used to compute energies for multiple states of the same symmetry. Benchmark applications of the new methods to the lowest valence (2)B(1) state of the allyl radical, low-lying states of the CH and CO(+) diatomics, and the nitromethyl radical show substantial improvement over ROHF- and UHF-based CCSD excitation energies for states with strong double-excitation character or cases suffering from significant spin contamination. For the allyl radical, CC3 adiabatic excitation energies differ from experiment by less than 0.02 eV, while for the (2)Sigma(+) state of CH, significant errors of more than 0.4 eV remain.

摘要

我们报告了耦合簇迭代三重态模型CC3对包括自由基在内的开壳层分子激发态的扩展。我们针对自旋非限制哈特里-福克(UHF)和自旋限制开壳层哈特里-福克(ROHF)参考行列式定义了该方法,并讨论了其在PSI3程序包中的高效实现。该程序经过简化,最多使用O(N(7))个计算步骤,并且在基态和激发态计算中都避免存储三重激发振幅。激发能程序利用了一种洛丁投影形式(与早期实现类似),该形式允许将戴维森算法的计算简化到仅单激发和双激发空间,但一次仅限制计算一个激发态。然而,可以使用根跟踪算法来计算相同对称性的多个态的能量。新方法在烯丙基自由基的最低价(2)B(1)态、CH和CO(+)双原子分子的低激发态以及硝基甲基自由基上的基准应用表明,对于具有强双激发特征的态或存在显著自旋污染的情况,与基于ROHF和UHF的CCSD激发能相比有了实质性的改进。对于烯丙基自由基,CC3绝热激发能与实验值的差异小于0.02 eV,而对于CH的(2)Σ(+)态,仍存在超过0.4 eV的显著误差。

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