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Exact Modified-Hartree-Fock scheme through perturbation expansion of density matrices

机译:通过扰动扩展密度矩阵的精确修正Hartree-Fock方案

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in the modified-Hartree-Fock (MHF) approach, as defined by Baroni and Tuncel (1983) (BT), the external potential is supplemented by a specific correlation potential, such that the density (determined with the HF method) of an N-electron system in this modified potential is the same as the ground-state density of the exact many-body solution for this system in the original potential. The MHF equations may be viewed as describing a model noninteracting N-electron system [analog of the Kohn-Sham (KS) system], moving in a one-body effective potential-the sum of three local terms: external, electrostatic, and BT correlation, and of the nonlocal HF exchange. The present study introduces an adiabatic link between the fully interacting system and this MHF noninteracting system by scaling the two-body electron-electron interaction with a factor a: in the range [0, 1], similarly as it was done by Levy and Perdew (1985) to link with the KS noninteracting system. An appropriate a-dependent functional F of the density n is defined using Levy constrained-search formulation of the density-functional theory. Density matrices serve as an indispensable tool. A term in F, representing the (1 - alpha) fraction of the electron repulsion energy, leads to an effective one-body nonlocal potential in an a-dependent Hamiltonian, the construction of which guarantees the density to be independent of or. Its ground-state solution serves for calculating F. This solution can be determined by means of the perturbation theory, with the unperturbed (alpha = 0) Hamiltonian generating the MHF determinantal wave function, in analogy to the Gorling and Levy (1993) approach with the KS function as the unperturbed one. Terms of the perturbation expansion for the BT correlation energy and potential can be calculated self-consistently in this way. Expressions for the BT correlation energy are obtained also in a form of integrals over the coupling parameter, involving a-dependent density matrices. (C) 1998 John Wiley & Sons, Inc. Int J Quant Chem 69: 469-483, 1998. [References: 27]
机译:在Baroni和Tuncel(1983)(BT)所定义的改良Hartree-Fock(MHF)方法中,外部电势由特定的相关电势进行补充,使得N的密度(由HF法确定) -在此修改后的电势中的电子系统与该系统在原始电势中的精确多体解的基态密度相同。 MHF方程可以看作描述了一个模型非相互作用的N电子系统[Kohn-Sham(KS)系统的模拟],它以一个整体的有效电势移动-三个局部项之和:外部,静电和BT相关性,以及非本地HF交换。本研究通过在[0,1]范围内缩放两体电子-电子相互作用,在完全相互作用的系统与该MHF非相互作用系统之间引入了绝热联系,类似于Levy和Perdew所做的那样。 (1985年)与KS非交互系统链接。使用密度泛函理论的Levy约束搜索公式定义密度n的适当的a依赖的函数F。密度矩阵是必不可少的工具。 F中的一项表示电子排斥能量的(1-α)分数,导致a依赖的哈密顿量中有效的单体非局部电势,该结构的构造保证了密度独立于或。它的基态解用于计算F。可以通过扰动理论来确定该解,其中无扰动(α= 0)的哈密顿量产生MHF行列式波函数,类似于Gorling和Levy(1993)的方法。 KS的功能一应俱全。可以以这种方式自洽地计算出BT相关能量和势的摄动展开项。 BT相关能量的表达式也可以通过耦合参数上的积分形式获得,涉及a依赖密度矩阵。 (C)1998 John Wiley&Sons,Inc. Int J Quant Chem 69:469-483,1998。[参考:27]

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