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用于半导体过渡金属化合物能带结构计算的杂化密度泛函理论+V方法:以二氧化铈为例

Hybrid-DFT  +  V method for band structure calculation of semiconducting transition metal compounds: the case of cerium dioxide.

作者信息

Ivády Viktor, Gali Adam, Abrikosov Igor A

机构信息

Department of Physics, Chemistry and Biology, Linköping University, SE-581 83 Linköping, Sweden. Wigner Research Centre for Physics, Hungarian Academy of Sciences, PO Box 49, H-1525, Budapest, Hungary.

出版信息

J Phys Condens Matter. 2017 Nov 15;29(45):454002. doi: 10.1088/1361-648X/aa8b93.

DOI:10.1088/1361-648X/aa8b93
PMID:28891806
Abstract

Hybrid functionals' non-local exchange-correlation potential contains a derivative discontinuity that improves on standard semi-local density functional theory (DFT) band gaps. Moreover, by careful parameterization, hybrid functionals can provide self-interaction reduced description of selected states. On the other hand, the uniform description of all the electronic states of a given system is a known drawback of these functionals that causes varying accuracy in the description of states with different degrees of localization. This limitation can be remedied by the orbital dependent exact exchange extension of hybrid functionals; the hybrid-DFT  +  V method (Ivády et al 2014 Phys. Rev. B 90 035146). Based on the analogy of quasi-particle equations and hybrid-DFT single particle equations, here we demonstrate that parameters of hybrid-DFT  +  V functional can be determined from approximate theoretical quasi-particle spectra without any fitting to experiment. The proposed method is illustrated on the charge self-consistent electronic structure calculation for cerium dioxide where itinerant valence states interact with well-localized 4f atomic like states, making this system challenging for conventional methods, either hybrid-DFT or LDA  +  U, and therefore allowing for a demonstration of the advantages of the proposed scheme.

摘要

杂化泛函的非局部交换关联势包含一个导数不连续性,这改进了标准半局部密度泛函理论(DFT)的带隙。此外,通过仔细的参数化,杂化泛函可以对选定状态提供减少自相互作用的描述。另一方面,对给定系统的所有电子态进行统一描述是这些泛函的一个已知缺点,这会导致对不同局域化程度的状态描述具有不同的准确性。这种限制可以通过杂化泛函的轨道相关精确交换扩展来弥补;即杂化密度泛函 + V 方法(伊瓦迪等人,《物理评论B》,2014年,第90卷,035146页)。基于准粒子方程和杂化密度泛函单粒子方程的类比,我们在此证明,杂化密度泛函 + V 泛函的参数可以从近似理论准粒子能谱中确定,而无需对实验进行任何拟合。在二氧化铈的电荷自洽电子结构计算中展示了所提出的方法,其中巡游价态与高度局域化的类4f原子态相互作用,这使得该系统对传统方法(无论是杂化密度泛函还是LDA + U)都具有挑战性,因此可以证明所提出方案的优势。

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