arXivDaily arXiv每日学术速递 周一至周五更新
arXiv 1608.07320physics.chem-phcond-mat.str-elphysics.comp-phquant-ph
收藏

基于DFT + $U$的自相互作用误差校正的精确约束和最小两参数推广的不适用性

Inapplicability of exact constraints and a minimal two-parameter generalization to the DFT+$U$ based correction of self-interaction error

Glenn Moynihan, Gilberto Teobaldi, David D. O'Regan

摘要:

在近似密度泛函理论中,自相互作用误差是与低估的绝缘间隙相关的电子离域异常。它表现出一个主要的二次能量密度曲线,可以使用有效的,类似约束的方法,如DFT + Hubbard $U$(DFT+ $U$)进行校正。约束DFT(cDFT)严格执行DFT上的条件,通过自洽优化的拉格朗日乘子,而它的使用自动化误差校正是一个令人信服的可能性,我们表明,它是有限的基本不相容的约束超出线性顺序。我们规避这个问题,利用单独的线性和二次校正项,这可以被解释为不同的约束,每个都有自己的哈伯德$U$型拉格朗日乘子,或作为一个广义DFT+ $U$功能的组件。后一种方法在我们对模型单电子系统$H_2^+$的测试中占主导地位,因为它很容易恢复精确的总能量,而保留能量的纯约束却不能做到这一点。广义DFT+ $U$泛函可以同时修正总能量和电离势,也可以修正Koopmans条件.对于后者的情况下,我们概述了一个实用的,近似的计划,所需的哈伯德参数,表示为U1和U2,可以计算从第一原理。

英文摘要:

In approximate density functional theory (DFT), the self-interaction error is an electron delocalization anomaly associated with underestimated insulating gaps. It exhibits a predominantly quadratic energy-density curve that is amenable to correction using efficient, constraint-resembling methods such as DFT + Hubbard $U$ (DFT+$U$). Constrained DFT (cDFT) enforces conditions on DFT exactly, by means of self-consistently optimized Lagrange multipliers, and while its use to automate error corrections is a compelling possibility, we show that it is limited by a fundamental incompatibility with constraints beyond linear order. We circumvent this problem by utilizing separate linear and quadratic correction terms, which may be interpreted either as distinct constraints, each with its own Hubbard $U$ type Lagrange multiplier, or as the components of a generalized DFT+$U$ functional. The latter approach prevails in our tests on a model one-electron system, $H_2^+$, in that it readily recovers the exact total-energy while symmetry-preserving pure constraints fail to do so. The generalized DFT+$U$ functional moreover enables the simultaneous correction of the total-energy and ionization potential or the correction of either together with the enforcement of Koopmans condition. For the latter case, we outline a practical, approximate scheme by which the required pair of Hubbard parameters, denoted as U1 and U2, may be calculated from first-principles.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

↑