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Ultra-nonlocality in density functional theory for photo-emission spectroscopy

机译:密度泛函理论在光发射光谱学中的超局域性

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摘要

We derive an exact expression for the photocurrent of photo-emission spectroscopy using timedependent current density functional theory (TDCDFT). This expression is given as an integral over the Kohn-Sham spectral function renormalized by effective potentials that depend on the exchange-correlation kernel of current density functional theory. We analyze in detail the physical content of this expression by making a connection between the density-functional expression and the diagrammatic expansion of the photocurrent within many-body perturbation theory. We further demonstrate that the density functional expression does not provide us with information on the kinetic energy distribution of the photo-electrons. Such information can, in principle, be obtained from TDCDFT by exactly modeling the experiment in which the photocurrent is split into energy contributions by means of an external electromagnetic field outside the sample, as is done in standard detectors. We find, however, that this procedure produces very nonlocal correlations between the exchange-correlation fields in the sample and the detector.
机译:我们使用时变电流密度泛函理论(TDCDFT)得出光发射光谱的光电流的精确表达式。该表达式作为由有效电势重新归一化的Kohn-Sham谱函数的积分给出,有效电势取决于电流密度泛函理论的交换相关核。我们通过在多体摄动理论中建立密度函数表达式与光电流的图解展开之间的联系来详细分析该表达式的物理内容。我们进一步证明,密度泛函表达式不能为我们提供有关光电子动能分布的信息。原则上,可以通过对实验进行精确建模来从TDCDFT中获得此类信息,在该实验中,光电流通过样品外部的外部电磁场分成能量贡献,就像在标准检测器中所做的那样。但是,我们发现此过程在样本和检测器的交换相关字段之间产生了非常非局部的相关性。

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