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A simple Semi-Explicit Density Functional Approach for Electron Systems

机译:电子系统的一种简单的半显式密度泛函方法

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摘要

One of the main reasons of the great impact of density-functional theory in the current research in physics and chemistry is the possibility of studying microscopically the structure of complex systems for which other quantum mechanical methods are not applicable. Most of the applications of DFT are performed via the Kohn-Sham equations, which appear when the energy functional depends on the density via a set of electron orbitals (implicit density functional), as opposed to the first functionals used in this theory which depend only on the density itself, like the Thomas-Fermi and Thomas-Fermi-Dirac (explicit density functionals). For the challenge of the study of very complex systems, where the Kohn-Sham equations might be difficult to apply, these explicit functionals could be the only alternative for an ab-initio calculation, because of their extreme simplicity. However, there are different failures in the models derived by them, such as the no-binding feature (Teller's theorem), the no possibility of describing negative ions, a loss of precision in the calculation of average properties and the difficulties found for the relativistic extensions.
机译:密度泛函理论在当前的物理和化学研究中产生巨大影响的主要原因之一是可以微观地研究不适用其他量子力学方法的复杂系统的结构。 DFT的大多数应用都是通过Kohn-Sham方程执行的,当能量函数通过一组电子轨道(隐式密度函数)依赖于密度时出现,这与该理论中仅依赖于该函数的第一个函数相反密度本身,例如Thomas-Fermi和Thomas-Fermi-Dirac(显式密度泛函)。对于研究可能很难应用Kohn-Sham方程的非常复杂的系统的挑战,由于它们极其简单,因此这些显式函数可能是ab-initio计算的唯一替代方法。但是,由它们推导的模型存在不同的故障,例如无结合特征(泰勒定理),不可能描述负离子,平均性能计算的精确度降低以及相对论发现的困难。扩展名。

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