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Multiconfiguration Pair-Density Functional Theory

机译:多配置对密度泛函理论

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We present a new theoretical framework, called Multiconfiguration Pair-Density Functional Theory (MC-PDFT), which combines multiconfigurational wave functions with a generalization of density functional theory (DFT). A multiconfigurational self-consistent-field (MCSCF) wave function with correct spin and space symmetry is used to compute the total electronic density, its gradient, the on-top pair density, and the kinetic and Coulomb contributions to the total electronic energy. We then use a functional of the total density, its gradient, and the on-top pair density to calculate the remaining part of the energy, which we call the on-top-density-functional energy in contrast to the exchange-correlation energy or Kohn—bham DM. Because the on-top pair density is an element or the two-particle density matrix, this goes beyond the Hohenberg—Kohn theorem that refers only to the one-particle density. To illustrate the theory, we obtain first approximations to the required new type of density functionals by translating conventional density functionals of the spin densities using a simple prescription, and we perform post-SCF density functional calculations using the total density, density gradient, and on-top pair density from the MCSCF calculations. Double counting of dynamic correlation or exchange does not occur because the MCSCF energy is not used. The theory is illustrated by applications to the bond energies and potential energy curves of H2, N2, F2, CaO, Cr^ and NiCl and the electronic excitation energies of Be, C, N, N~+, O, O~+, Sc~+, Mn, Co, Mo, Ru, N2, HCHO, C4H6, c-CsH6, and pyrazine. The method presented has a computational cost and scaling similar to MCSCF, but a quantitative accuracy, even with the present first approximations to the new types of density functionals, that is comparable to much more expensive multireference perturbation theory methods.
机译:我们提出了一种新的理论框架,称为多配置对密度泛函理论(MC-PDFT),该框架结合了多配置波动函数和密度泛函理论(DFT)的概括。具有正确的自旋和空间对称性的多配置自洽场(MCSCF)波函数用于计算总电子密度,其梯度,顶对密度以及对总电子能量的动力学和库仑贡献。然后,我们使用总密度,梯度和顶部对密度的函数来计算能量的剩余部分,我们将其称为顶部密度函数能量,而不是交换相关能量或Kohn-bham DM。由于顶对密度是元素或两粒子密度矩阵,因此这超出了仅指单粒子密度的Hohenberg-Kohn定理。为了说明该理论,我们通过使用简单的公式平移自旋密度的常规密度泛函来获得所需新型密度泛函的第一近似值,然后使用总密度,密度梯度等对SCF进行密度函数计算。 -MCSCF计算得出的最高对对密度。由于未使用MCSCF能量,因此不会发生动态相关或交换的重复计数。将该理论应用于H2,N2,F2,CaO,Cr ^和NiCl的键能和势能曲线以及Be,C,N,N〜+,O,O〜+,Sc的电子激发能〜+,Mn,Co,Mo,Ru,N2,HCHO,C4H6,c-CsH6和吡嗪。所提出的方法具有类似于MCSCF的计算成本和缩放比例,但是即使在目前对新型密度泛函类型进行初次近似的情况下,其定量精度仍可与更昂贵的多参考微扰理论方法相媲美。

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