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On extending Kohn-Sham density functionals to systems with fractional number of electrons

机译:关于将Kohn-Sham密度泛函扩展为具有分数电子的系统

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摘要

We analyze four ways of formulating the Kohn-Sham (KS) density functionals with a fractional number of electrons, through extending the constrained search space from the Kohn-Sham and the generalized Kohn-Sham (GKS) non-interacting v-representable density domain for integer systems to four different sets of densities for fractional systems. In particular, these density sets are (I) ensemble interacting N-representable densities, (II) ensemble non-interacting N-representable densities, (III) non-interacting densities by the Janak construction, and (IV) non-interacting densities whose composing orbitals satisfy the Aufbau occupation principle. By proving the equivalence of the underlying first order reduced density matrices associated with these densities, we show that sets (I), (II), and (III) are equivalent, and all reduce to the Janak construction. Moreover, for functionals with the ensemble v-representable assumption at the minimizer, (III) reduces to (IV) and thus justifies the previous use of the Aufbau protocol within the (G)KS framework in the study of the ground state of fractional electron systems, as defined in the grand canonical ensemble at zero temperature. By further analyzing the Aufbau solution for different density functional approximations (DFAs) in the (G)KS scheme, we rigorously prove that there can be one and only one fractional occupation for the Hartree Fock functional, while there can be multiple fractional occupations for general DFAs in the presence of degeneracy. This has been confirmed by numerical calculations using the local density approximation as a representative of general DFAs. This work thus clarifies important issues on density functional theory calculations for fractional electron systems.
机译:我们通过扩展Kohn-Sham和广义Kohn-Sham(GKS)非相互作用的v可表示密度域的约束搜索空间,分析了用分数个电子来表示Kohn-Sham(KS)密度泛函的四种方式对于整数系统而言,对于分数系统而言是四种不同的密度集。特别地,这些密度集是(I)整体相互作用的N可表示的密度,(II)整体不可相互作用的N可表示的密度,(III)通过Janak结构的非相互作用的密度,以及(IV)其相互作用的密度组成轨道符合Aufbau占领原则。通过证明与这些密度相关的底层一阶降低密度矩阵的等价关系,我们证明了集合(I),(II)和(III)是等效的,并且全部归结为Janak构造。此外,对于在最小化器处具有整体v可表示假设的函数,(III)还原为(IV),因此证明了先前在(G)KS框架内使用Aufbau协议进行分数电子基态研究的合理性系统,如零温度下的大典范合奏中所定义。通过进一步分析(G)KS方案中不同密度泛函近似(DFA)的Aufbau解,我们严格证明了Hartree Fock泛函可以只有一个分数职业,而对于一般密度函数可以有多个分数职业。存在简并性的DFA。这已通过使用局部密度近似值代表一般DFA的数值计算得到了证实。因此,这项工作阐明了关于分数电子系统的密度泛函理论计算的重要问题。

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