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Levy-Lieb-Based Monte Carlo Study of the Dimensionality Behaviour of the Electronic Kinetic Functional

机译:基于Levy-Lieb的蒙特卡罗电子动力学功能的维数行为研究

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We consider a gas of interacting electrons in the limit of nearly uniform density and treat the one dimensional (1D), two dimensional (2D) and three dimensional (3D) cases. We focus on the determination of the correlation part of the kinetic functional by employing a Monte Carlo sampling technique of electrons in space based on an analytic derivation via the Levy-Lieb constrained search principle. Of particular interest is the question of the behaviour of the functional as one passes from 1D to 3D; according to the basic principles of Density Functional Theory (DFT) the form of the universal functional should be independent of the dimensionality. However, in practice the straightforward use of current approximate functionals in different dimensions is problematic. Here, we show that going from the 3D to the 2D case the functional form is consistent (concave function) but in 1D becomes convex; such a drastic difference is peculiar of 1D electron systems as it is for other quantities. Given the interesting behaviour of the functional, this study represents a basic first-principle approach to the problem and suggests further investigations using highly accurate (though expensive) many-electron computational techniques, such as Quantum Monte Carlo.
机译:我们考虑在接近均匀密度的极限下与电子相互作用的气体,并处理一维(1D),二维(2D)和三维(3D)情况。我们着重于通过基于Levy-Lieb约束搜索原理的解析推导,采用空间中电子的蒙特卡洛采样技术确定动力学函数的相关部分。当人们从1D转换到3D时,功能的行为问题尤其令人关注。根据密度泛函理论(DFT)的基本原理,通用泛函的形式应独立于维。然而,在实践中,直接在不同维度上使用当前的近似功能是有问题的。在这里,我们显示了从3D到2D的情况下,功能形式是一致的(凹函数),但在1D情况下,它是凸的;一维电子系统的这种巨大差异与其他数量的电子系统一样。考虑到该功能的有趣行为,本研究代表了解决该问题的基本第一原理方法,并建议使用高精度(尽管价格昂贵)的多电子计算技术(例如量子蒙特卡洛)进行进一步的研究。

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