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基于均匀电子气交换关联空穴的对称非局部加权密度近似

Symmetric Nonlocal Weighted Density Approximations from the Exchange-Correlation Hole of the Uniform Electron Gas.

作者信息

Cuevas-Saavedra Rogelio, Chakraborty Debajit, Rabi Sandra, Cárdenas Carlos, Ayers Paul W

机构信息

Department of Chemistry and Chemical Biology, McMaster University , Hamilton, Ontario, Canada.

Departamento de Física, Facultad de Ciencias, Universidad de Chile , 653-Santiago, Chile.

出版信息

J Chem Theory Comput. 2012 Nov 13;8(11):4081-93. doi: 10.1021/ct300325t. Epub 2012 Nov 1.

Abstract

Nonlocal exchange-correlation energy functionals are constructed using the accurate model exchange-correlation hole for the uniform electron gas developed by Gori-Giorgi and Perdew. The exchange-correlation hole is constrained to be symmetric and normalized, so the resulting functionals can be viewed as symmetrized versions of the weighted density approximation; we call them two-point weighted density approximations. Even without optimization of parameters or functional forms, the exchange-correlation energies for small molecules are competitive with those of the best generalized gradient approximation functionals. Two-point weighted density approximations seem to be an interesting new direction for functional development. A more general version of the conditions that define the energy for fractional electron number and fractional spin are presented. These "generalized flat-planes" conditions are closely linked to the normalization of the spin-resolved exchange-correlation hole at noninteger electron number. This and many other properties of the exact exchange-correlation functional can be imposed straightforwardly and directly in symmetrized weighted density approximation.

摘要

非局域交换关联能泛函是利用Gori-Giorgi和Perdew为均匀电子气所开发的精确模型交换关联空穴构建的。交换关联空穴被约束为对称且归一化的,因此所得的泛函可被视为加权密度近似的对称化版本;我们将它们称为两点加权密度近似。即使不进行参数或泛函形式的优化,小分子的交换关联能也能与最佳广义梯度近似泛函的交换关联能相竞争。两点加权密度近似似乎是泛函发展的一个有趣的新方向。本文给出了定义分数电子数和分数自旋能量的条件的更一般版本。这些“广义平面”条件与非整数电子数下自旋分辨交换关联空穴的归一化密切相关。精确交换关联泛函的这一性质以及许多其他性质可以直接且直接地施加于对称化加权密度近似中。

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