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激发态的局域双自然轨道。

Local pair natural orbitals for excited states.

机构信息

Lehrstuhl für Theoretische Chemie, Ruhr-Universität Bochum, 44801 Bochum, Germany.

出版信息

J Chem Phys. 2011 Dec 7;135(21):214106. doi: 10.1063/1.3664902.

DOI:10.1063/1.3664902
PMID:22149778
Abstract

We explore how in response calculations for excitation energies with wavefunction based (e.g., coupled cluster) methods the number of double excitation amplitudes can be reduced by means of truncated pair natural orbital (PNO) expansions and localized occupied orbitals. Using the CIS(D) approximation as a test model, we find that the number of double excitation amplitudes can be reduced dramatically with minor impact on the accuracy if the excited state wavefunction is expanded in state-specific PNOs generated from an approximate first-order guess wavefunction. As for ground states, the PNO truncation error can also for excitation energies be controlled by a single threshold related to generalized natural occupation numbers. The best performance is found with occupied orbitals which are localized by the Pipek-Mezey localization. For a large test set of excited states we find with this localization that already a PNO threshold of 10(-8)-10(-7), corresponding to an average of only 40-80 PNOs per pair, is sufficient to keep the PNO truncation error for vertical excitation energies below 0.01 eV. This is a significantly more rapid convergence with the number doubles amplitudes than in domain-based local response approaches. We demonstrate that the number of significant excited state PNOs scales asymptotically linearly with the system size in the worst case of completely delocalized excitations and sub-linearly whenever the chromophore does not increase with the system size. Moreover, we observe that the flexibility of state-specific PNOs to adapt to the character of an excitation allows for an almost unbiased treatment of local, delocalized and charge transfer excited states.

摘要

我们探讨了如何通过截断对自然轨道(PNO)展开和定域占据轨道的双激发振幅来减少基于波函数(例如,耦合簇)方法的激发能的响应计算中的双激发振幅数。使用 CIS(D) 近似作为测试模型,我们发现如果将激发态波函数展开为来自近似一阶猜测波函数的状态特定 PNO,则可以大大减少双激发振幅数,而对准确性的影响很小。对于基态,PNO 截断误差也可以通过与广义自然占据数相关的单个阈值来控制激发能。通过 Pipek-Mezey 定域化的占据轨道可以获得最佳性能。对于一个大的激发态测试集,我们发现使用这种定域化,PNO 阈值为 10(-8)-10(-7),对应于平均每个对只有 40-80 个 PNO,足以将垂直激发能的 PNO 截断误差保持在 0.01 eV 以下。与基于域的局部响应方法相比,这是一种与双振幅数更快的收敛。我们证明,在完全离域激发的最坏情况下,显著激发态 PNO 的数量与系统大小呈渐近线性缩放,并且只要发色团不随系统大小增加,就呈次线性缩放。此外,我们观察到,状态特定 PNO 适应激发特性的灵活性允许对局部、离域和电荷转移激发态进行几乎无偏处理。

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