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二胺阳离子中的电荷定域为能量泛函和自相互作用校正提供了一个检验。

Charge localization in a diamine cation provides a test of energy functionals and self-interaction correction.

作者信息

Cheng Xinxin, Zhang Yao, Jónsson Elvar, Jónsson Hannes, Weber Peter M

机构信息

Department of Chemistry, Brown University, 324 Brook Street, Providence, Rhode Island 02912, USA.

COMP, Department of Applied Physics, Aalto University, FIN-00076 Espoo, Finland.

出版信息

Nat Commun. 2016 Mar 16;7:11013. doi: 10.1038/ncomms11013.

Abstract

Density functional theory (DFT) is widely applied in calculations of molecules and materials. Yet, it suffers from a well-known over-emphasis on charge delocalization arising from self-interaction error that destabilizes localized states. Here, using the symmetric diamine N,N'-dimethylpiperazine as a model, we have experimentally determined the relative energy of a state with positive charge localized on one of the two nitrogen atoms, and a state with positive charge delocalized over both nitrogen atoms. The charge-localized state was found to be 0.33 (0.04) eV higher in energy than the charge-delocalized state. This provides an important test of theoretical approaches to electronic structure calculations. Calculations with all DFT functionals commonly used today, including hybrid functionals with exact exchange, fail to predict a stable charge-localized state. However, the application of an explicit self-interaction correction to a semi-local functional identifies both states and gives relative energy in excellent agreement with both experiment and CCSD(T) calculations.

摘要

密度泛函理论(DFT)在分子和材料计算中得到广泛应用。然而,它存在一个众所周知的问题,即由于自相互作用误差导致对电荷离域的过度强调,从而使局域态不稳定。在此,我们以对称二胺N,N'-二甲基哌嗪为模型,通过实验确定了正电荷局域在两个氮原子之一上的状态与正电荷在两个氮原子上离域的状态的相对能量。结果发现,电荷局域态的能量比电荷离域态高0.33(0.04)电子伏特。这为电子结构计算的理论方法提供了重要检验。使用当今常用的所有DFT泛函进行计算,包括具有精确交换的杂化泛函,都无法预测稳定的电荷局域态。然而,对半局域泛函应用显式自相互作用校正可以识别这两种状态,并给出与实验和CCSD(T)计算都非常吻合的相对能量。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b7ff/4799366/8ea05d20d11c/ncomms11013-f1.jpg

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