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Construction of Fermi Potentials from Electronic Wave Functions

机译:电子波函数的FERMI电位构建

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The Fermi potential, v(F)(r), is the nonclassical part of the multiplicative effective potential appearing in the one-particle Schrodinger-type equation for the square root of the electron density. The usual way of constructing v(F)(r) by inverting that equation produces unsatisfactory results when applied to electron densities expanded in Gaussian basis sets. We suggest a different method that is based on an explicit formula for v(F)(r) in terms of the interacting one- and two-electron reduced density matrices of the system. This method is exact in the basis set limit and yields accurate approximations to the basis-set-limit v(F)(r) when applied to reduced density matrices represented in terms of finite basis sets. Illustrative applications involve atomic and molecular wave functions generated at various levels of ab initio theory. It is also shown how to construct the Pauli and exchange-correlation potentials of any system starting with only v(F)(r).
机译:费米势v(F)(r)是电子密度平方根的单粒子薛定谔型方程中乘法有效势的非经典部分。当应用于在高斯基集中展开的电子密度时,通常通过反转该方程来构造v(F)(r)的方法会产生不令人满意的结果。我们提出了一种不同的方法,该方法基于一个显式的v(F)(r)公式,即系统的相互作用的单电子和双电子约化密度矩阵。这种方法在基集极限中是精确的,当应用于以有限基集表示的约化密度矩阵时,可以得到基集极限v(F)(r)的精确近似值。说明性应用包括原子和分子波函数在从头算理论的不同层次上产生。文中还给出了如何构造仅从v(F)(r)开始的任何系统的泡利关联势和交换关联势。

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