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锰(III)自旋交叉配合物分子几何中分散性的重要性。

Importance of Dispersion in the Molecular Geometries of Mn(III) Spin-Crossover Complexes.

机构信息

Department of Chemistry, University of South Dakota, Vermillion, South Dakota 57069, United States.

出版信息

J Phys Chem A. 2023 Apr 13;127(14):3072-3081. doi: 10.1021/acs.jpca.2c08158. Epub 2023 Apr 3.

DOI:10.1021/acs.jpca.2c08158
PMID:37010904
Abstract

The computational investigation of the molecular geometries of a pair of manganese(III) spin-crossover complexes is reported. For the geometry of the quintet high-spin state, density functionals significantly overestimate Mn-N bond distances, although the geometry for the triplet intermediate-spin state is well described. Comparisons with several wave function-based methods demonstrate that this error is due to the limited ability of commonly used density functionals to recover dispersion beyond a certain extent. Among the methods employed for geometry optimization, restricted open-shell Møller-Plesset perturbation theory (MP2) appropriately describes the high-spin geometry but results in a slightly shorter Mn-O distance in both spin states. On the other hand, extended multistate complete active space second-order perturbation theory (XMS-CASPT2) provides a good description of the geometry for the intermediate-spin state but also sufficiently recovers dispersion, performing well for the high-spin state. Despite the fact that the electronic structure of both spin states is dominated by one-electron configuration, XMS-CASPT2 offers a balanced approach, leading to molecular geometries with much better agreement with experiment than MP2 and DFT. A scan along the Mn-N bond demonstrates that for these complexes coupled cluster methods (i.e., DLPNO-CCSD(T)) also yield bond distances in agreement with experiment while multiconfiguration pair density functional theory (MC-PDFT) is unable to recover dispersion well enough, analogous to single-reference DFT.

摘要

报道了一对锰(III)自旋交叉配合物分子几何形状的计算研究。对于 quintet high-spin 状态的几何形状,密度泛函法显著高估了 Mn-N 键距离,尽管 triplet intermediate-spin 状态的几何形状得到了很好的描述。与几种基于波函数的方法的比较表明,这种误差是由于常用密度泛函法在一定程度上恢复色散的能力有限。在用于几何优化的方法中,限制开壳层 Møller-Plesset 微扰理论(MP2)适当地描述了高自旋几何形状,但在两种自旋状态下都导致 Mn-O 距离略短。另一方面,扩展多态完全活性空间二级微扰理论(XMS-CASPT2)为中间自旋状态的几何形状提供了很好的描述,并且还充分恢复了色散,在高自旋状态下表现良好。尽管两种自旋状态的电子结构都由单电子构型主导,但 XMS-CASPT2 提供了一种平衡的方法,导致分子几何形状与实验更吻合,优于 MP2 和 DFT。沿着 Mn-N 键的扫描表明,对于这些配合物,耦合簇方法(即 DLPNO-CCSD(T))也产生与实验一致的键距离,而多组态对密度泛函理论(MC-PDFT)无法很好地恢复色散,类似于单参考 DFT。

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