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应用于[(PYMe)MoO]配合物的KID程序。

KID Procedure Applied on the [(PYMe)MoO] Complex.

作者信息

Glossman-Mitnik Daniel, Martínez-Araya Jorge I

机构信息

Laboratorio Virtual NANOCOSMOS, Departamento de Medio Ambiente y Energía, Centro de Investigación en Materiales Avanzados, Chihuahua, Chih 31136, Mexico.

Departamento de Ciencias Químicas, Facultad de Ciencias Exactas, Universidad Andres Bello (UNAB), Av. República 498, Santiago 8370146, Chile.

出版信息

ACS Omega. 2020 Nov 16;5(47):30549-30555. doi: 10.1021/acsomega.0c04450. eCollection 2020 Dec 1.

Abstract

The KID (Koopmans in DFT) protocol usually applies in organic molecules of the closed-shell type. We used the KID procedure on an open-shell Mo-based system for the first time to choose the most suitable density functional to compute global and local reactivity descriptors obtained from the conceptual density-functional theory (DFT). From a set of 18 density functionals, spread from the second until the fourth rung of Jacob's ladder: BLYP, BP86, B97-D, MN12-L, MN15-L, M06-L, M11-L, CAM-B3LYP, PBE0, B3LYP, N12-SX, M06-2X, MN15, MN12-SX, ωB97X-D, M11, LC-ωHPBE, and APFD, we concluded that CAM-B3LYP provides the best outcome, and in the second place, M06-2X. Because the vertical first ionization potential and vertical first electron affinity in the ground state (gs) are defined as follows = ( - 1) - () and = () - ( + 1), where ( - 1), (), and ( + 1) correspond to energies of the system bearing , + 1, and - 1 electrons, along with Koopmans' theorem (KT) given by ≈ -ε (ε, highest occupied molecular orbital energy) and ≈ -ε (ε, lowest unoccupied molecular orbital energy), the deviation from the KT was performed by the use of the index, such that = | ( - 1) - () + ε| and = | () - ( + 1) + ε|, which are absolute deviations from the perspective of and , respectively. Furthermore, the ε (SOMO: singly-occupied molecular orbital energy) leads us to another index given by |ΔSL| = |ε - ε|. Therefore, and |ΔSL| are indexes defined to evaluate the quality of the KT when employed within the context of quantum chemical calculations based on DFT and not the Hartree-Fock theory. We propose the index that could be more suitable to choose the most proper density functional because the and |ΔSL| are independent indexes.

摘要

KID(密度泛函理论中的库普曼斯方法)协议通常适用于闭壳层类型的有机分子。我们首次在开壳层的钼基体系上使用KID程序,以选择最合适的密度泛函来计算从概念密度泛函理论(DFT)获得的全局和局部反应性描述符。从一组18种密度泛函中进行选择,这些密度泛函分布在雅各布天梯的第二级到第四级:BLYP、BP86、B97-D、MN12-L、MN15-L、M06-L、M11-L、CAM-B3LYP、PBE0、B3LYP、N12-SX、M06-2X、MN15、MN12-SX、ωB97X-D、M11、LC-ωHPBE和APFD,我们得出结论,CAM-B3LYP给出的结果最佳,其次是M06-2X。由于基态(gs)下的垂直第一电离势和垂直第一电子亲和能定义如下:(I = E(N - 1) - E(N)) 和 (A = E(N) - E(N + 1)),其中 (E(N - 1))、(E(N)) 和 (E(N + 1)) 分别对应体系带有 (N)、(N + 1) 和 (N - 1) 个电子时的能量,再结合由 (I \approx -\varepsilon_{HOMO})((\varepsilon_{HOMO}),最高占据分子轨道能量)和 (A \approx -\varepsilon_{LUMO})((\varepsilon_{LUMO}),最低未占据分子轨道能量)给出的库普曼斯定理(KT),通过使用该指数来计算与KT的偏差,使得 (D_{I} = |E(N - 1) - E(N)+\varepsilon_{HOMO}|) 和 (D_{A} = |E(N) - E(N + 1)+\varepsilon_{LUMO}|),它们分别是从 (I) 和 (A) 的角度出发的绝对偏差。此外((\varepsilon_{SOMO}):单占据分子轨道能量) 使我们得到另一个指数 (|\Delta S_{L}| = |\varepsilon_{SOMO}-\varepsilon_{LUMO}|)。因此,(D_{I}) 和 (|\Delta S_{L}|) 是在基于DFT而非哈特里−福克理论的量子化学计算背景下用于评估KT质量的指数。我们提出这个可能更适合选择最合适密度泛函的指数,因为 (D_{I}) 和 (|\Delta S_{L}|) 是相互独立的指数。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/edf0/7711706/71f92fdb48a2/ao0c04450_0002.jpg

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