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带有自旋轨道耦合的开壳重元素体系的耦合簇方法。

Coupled-cluster method for open-shell heavy-element systems with spin-orbit coupling.

机构信息

Institute of Atomic and Molecular Physics, Key Laboratory of High Energy Density Physics and Technology, Ministry of Education, Sichuan University, Chengdu 610065, People's Republic of China.

出版信息

J Chem Phys. 2017 Apr 7;146(13):134108. doi: 10.1063/1.4979491.

Abstract

The coupled-cluster approach with spin-orbit coupling (SOC) included in post-self-consistent field treatment (SOC-CC) using relativistic effective core potentials is extended to spatially non-degenerate open-shell systems in this work. The unrestricted Hartree-Fock determinant corresponding to the scalar relativistic Hamiltonian is employed as the reference and the open-shell SOC-CC approach is implemented at the CC singles and doubles (CCSD) level as well as at the CCSD level augmented by a perturbative treatment of triple excitations (CCSD(T)). Due to the breaking of time-reversal symmetry and spatial symmetry, this open-shell SOC-CC approach is rather expensive compared with the closed-shell SOC-CC approach. The open-shell SOC-CC approach is applied to some open-shell atoms and diatomic molecules with s, p, σ, or π configuration. Our results indicate that rather accurate results can be achieved with the open-shell SOC-CCSD(T) approach for these systems. Dissociation energies for some closed-shell molecules containing heavy IIIA or VIIA atoms are also calculated using the closed-shell SOC-CC approach, where energies of the IIIA or VIIA atoms are obtained from those of the closed-shell ions and experimental ionization potentials or electron affinities. SOC-CCSD(T) approach affords reliable dissociation energies for these molecules. Furthermore, scalar-relativistic CCSD(T) approach with the same strategy can also provide reasonable dissociation energies for the 5th row IIIA or VIIA molecules, while the error becomes pronounced for the 6th row elements.

摘要

本工作中,在自洽场处理后(SOC-CC)中纳入自旋轨道耦合(SOC)的耦合簇方法扩展到了空间非简并的开壳层体系。采用与标量相对论哈密顿量对应的非限制哈特利-福克行列式作为参考,在 CC 单激发和双激发(CCSD)水平以及通过微扰处理三重激发(CCSD(T))加以增强的 CCSD 水平上实现了开壳层 SOC-CC 方法。由于时间反演对称性和空间对称性的破坏,与闭壳层 SOC-CC 方法相比,这种开壳层 SOC-CC 方法的开销相当大。我们将开壳层 SOC-CC 方法应用于一些具有 s、p、σ 或π构型的开壳层原子和双原子分子。结果表明,对于这些体系,采用开壳层 SOC-CCSD(T)方法可以获得相当准确的结果。我们还使用闭壳层 SOC-CC 方法计算了一些含有 IIIA 或 VIIA 重原子的闭壳层分子的离解能,其中 IIIA 或 VIIA 原子的能量取自闭壳层离子以及实验电离势或电子亲合势。SOC-CCSD(T)方法为这些分子提供了可靠的离解能。此外,采用相同策略的标量相对论 CCSD(T)方法也可以为第五周期 IIIA 或 VIIA 分子提供合理的离解能,而对于第六周期元素,误差变得显著。

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