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一种仅使用从头算数据参数化的密度泛函理论/多参考组态相互作用哈密顿量:I. 价层激发态。

A DFT/MRCI Hamiltonian parameterized using only ab initio data: I. valence excited states.

作者信息

Costain Teagan Shane, Ogden Victoria, Neville Simon P, Schuurman Michael S

机构信息

Department of Chemistry and Biomolecular Sciences, University of Ottawa, Ottawa, Ontario K1N 6N5, Canada.

National Research Council Canada, 100 Sussex Dr., Ottawa, Ontario K1A 0R6, Canada.

出版信息

J Chem Phys. 2024 Jun 14;160(22). doi: 10.1063/5.0210897.

Abstract

A new combined density functional theory and multi-reference configuration interaction (DFT/MRCI) Hamiltonian parameterized solely using the benchmark ab initio vertical excitation energies obtained from the QUEST databases is presented. This new formulation differs from all previous versions of the method in that the choice of the underlying exchange-correlation (XC) functional employed to construct the one-particle (orbital) basis is considered, and a new XC functional, QTP17, is chosen for its ability to generate a balanced description of core and valence vertical excitation energies. The ability of the new DFT/MRCI Hamiltonian, termed QE8, to furnish accurate excitation energies is confirmed using benchmark quantum chemistry computations, and a mean absolute error of 0.16 eV is determined for the wide range of electronic excitations included in the validation dataset. In particular, the QE8 Hamiltonian dramatically improves the performance of DFT/MRCI for doubly excited states. The performance of fast approximate DFT/MRCI methods, p-DFT/MRCI and DFT/MRCI(2), is also evaluated using the QE8 Hamiltonian, and they are found to yield excitation energies in quantitative agreement with the parent DFT/MRCI method, with the two methods exhibiting a mean difference of 0.01 eV with respect to DFT/MRCI over the entire benchmark set.

摘要

提出了一种新的结合密度泛函理论和多参考组态相互作用(DFT/MRCI)的哈密顿量,该哈密顿量仅使用从QUEST数据库获得的基准从头算垂直激发能进行参数化。这种新的公式与该方法的所有先前版本不同之处在于,考虑了用于构建单粒子(轨道)基的基础交换相关(XC)泛函的选择,并且选择了一种新的XC泛函QTP17,因为它能够对核心和价层垂直激发能产生平衡的描述。使用基准量子化学计算证实了新的DFT/MRCI哈密顿量(称为QE8)提供精确激发能的能力,并确定了验证数据集中包含的广泛电子激发的平均绝对误差为0.16 eV。特别是,QE8哈密顿量显著提高了DFT/MRCI对双激发态的性能。还使用QE8哈密顿量评估了快速近似DFT/MRCI方法p-DFT/MRCI和DFT/MRCI(2)的性能,发现它们产生的激发能与原始DFT/MRCI方法在数量上一致,在整个基准集上,这两种方法相对于DFT/MRCI的平均差异为0.01 eV。

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