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含时密度泛函和格林函数方法在自由基激发能及里德堡电子态计算中的性能

Performance of time-dependent density functional and Green functions methods for calculations of excitation energies in radicals and for Rydberg electronic states.

作者信息

Zyubin A S, Mebel A M

机构信息

Institute of Atomic and Molecular Sciences, Academia Sinica, P.O. Box 23-166, Taipei 106, Taiwan, Republic of China.

出版信息

J Comput Chem. 2003 Apr 30;24(6):692-700. doi: 10.1002/jcc.10220.

Abstract

Time-dependent density functional (TD-DFT) and perturbation theory-based outer valence Green functions (OVGF) methods have been tested for calculations of excitation energies for a set of radicals, molecules, and model clusters simulating points defects in silica. The results show that the TD-DFT approach may give unreliable results not only for diffuse Rydberg states, but also for electronic states involving transitions between MOs localized in two remote from each other spatial regions, for example, for charge-transfer excitations. For the. O-SiX(3) clusters, where X is a single-valence group, TD-DFT predicts reasonable excitation energies but incorrect sequence of electronic transitions. For a number of cases where TD-DFT is shown to be unreliable, the OVGF approach can provide better estimates of excitation energies, but this method also is not expected to perform universally well. The OVGF performance is demonstrated to be satisfactory for excitations with predominantly single-determinant wave functions where the deviations of the calculated energies from experiment should not exceed 0.1-0.3 eV. However, for more complicated transitions involving multiple bonds or for excited states with multireference wave functions the OVGF approach is less reliable and error in the computed energies can reach 0.5-1 eV.

摘要

基于含时密度泛函理论(TD-DFT)和微扰理论的价层格林函数(OVGF)方法,已针对一组模拟二氧化硅中点缺陷的自由基、分子和模型团簇的激发能计算进行了测试。结果表明,TD-DFT方法不仅对于漫射里德堡态可能给出不可靠的结果,而且对于涉及位于彼此相距较远的两个空间区域中的分子轨道之间跃迁的电子态,例如对于电荷转移激发,也可能给出不可靠的结果。对于O-SiX(3)团簇(其中X为单价基团),TD-DFT预测了合理的激发能,但电子跃迁顺序不正确。在许多TD-DFT被证明不可靠的情况下,OVGF方法可以提供更好的激发能估计,但该方法也并非在所有情况下都能表现良好。对于主要具有单行列式波函数的激发,OVGF的性能被证明是令人满意的,此时计算能量与实验值的偏差不应超过0.1 - 0.3 eV。然而,对于涉及多个键的更复杂跃迁或具有多参考波函数的激发态,OVGF方法不太可靠,计算能量的误差可达0.5 - 1 eV。

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