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用于估算负电子亲和势的简单密度泛函理论方案。

Simple DFT Scheme for Estimating Negative Electron Affinities.

作者信息

Vibert Christopher P, Tozer David J

机构信息

Department of Chemistry , Durham University , South Road , Durham , DH1 3LE U.K.

出版信息

J Chem Theory Comput. 2019 Jan 8;15(1):241-248. doi: 10.1021/acs.jctc.8b00938. Epub 2018 Dec 12.

DOI:10.1021/acs.jctc.8b00938
PMID:30495952
Abstract

A simple density functional theory (DFT) scheme is proposed for estimating negative vertical electron affinities of neutral systems, based on a consideration of the integer discontinuity and density scaling homogeneity. The key feature is the derivation of two system-dependent exchange-correlation functionals, one appropriate for the electron deficient side of the integer and one appropriate for the electron abundant side. The electron affinity is evaluated as a linear combination of frontier orbital energies from self-consistent Kohn-Sham calculations on the neutral system using these functionals. For two assessments comprising a total of 43 molecules, the scheme provides electron affinities that are in good agreement with experimental values and which are an improvement over those from the DFT method of Tozer and De Proft [ J. Phys. Chem. A 2005 , 109 , 8923 ]. The scheme is trivial to implement in any Kohn-Sham program, and the computational cost is that of a series of generalized gradient approximation Kohn-Sham calculations. More generally, the study provides a prescription for performing low-cost, self-consistent Kohn-Sham calculations that yield frontier orbital energies that approximately satisfy the appropriate Koopmans conditions, without the need for exact exchange.

摘要

基于对整数间断性和密度缩放均匀性的考虑,提出了一种简单的密度泛函理论(DFT)方案来估算中性体系的负垂直电子亲和能。其关键特性是推导了两个与体系相关的交换相关泛函,一个适用于整数的电子缺乏侧,另一个适用于电子丰富侧。使用这些泛函,通过对中性体系进行自洽的Kohn-Sham计算,将电子亲和能评估为前沿轨道能量的线性组合。对于总共包含43个分子的两项评估,该方案提供的电子亲和能与实验值高度吻合,并且比Tozer和De Proft的DFT方法[《物理化学杂志A》2005年,109卷,8923页]所得结果有所改进。该方案在任何Kohn-Sham程序中都易于实现,计算成本为一系列广义梯度近似Kohn-Sham计算的成本。更一般地说,该研究提供了一种进行低成本、自洽Kohn-Sham计算的方法,该计算能产生近似满足适当Koopmans条件的前沿轨道能量,而无需精确交换。

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