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Using multipole point charge distributions to provide the electrostatic potential in the variational explicit polarization (X-Pol) potential

机译:使用多极点电荷分布在变显性极化(X-Pol)电势中提供静电势

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The equations defining the variational explicit polarization (X-Pol) potential introduced in earlier work are modified in the present work so that multipole point charge distributions are used instead of Mulliken charges to polarize the monomers that comprise the system. In addition, when computing the electrostatic interaction between a monomer whose molecular orbitals are being optimized and a monomer whose electron density is being used to polarize the first monomer, the electron densities of both monomers are represented by atom-centered multipole point charge distributions. In the original formulation of the variational X-Pol potential, the continuous electron density of the monomer being optimized interacts with external Mulliken charges, but this corresponds to the monopole truncation in a multipole expansion scheme in the computation of the Fock matrix elements of the given monomer. The formulation of the variational X-Pol potential introduced in this work (which we are calling the "multi-pole variational X-Pol potential") represents the electron density of the monomer whose wave function is being variationally optimized in the same way that it represents the electron densities of external monomers when computing the Coulomb interactions between them.
机译:在较早的工作中引入了定义变异显性极化(X-Pol)电势的方程式,在本工作中对此进行了修改,以便使用多极点电荷分布代替Mulliken电荷来极化构成系统的单体。另外,当计算分子轨道被优化的单体与电子密度用于使第一单体极化的单体之间的静电相互作用时,两种单体的电子密度均以原子为中心的多极点电荷分布表示。在X-Pol电位变化的原始公式中,被优化的单体的连续电子密度与外部Mulliken电荷相互作用,但这对应于给定Fock矩阵元素的计算中的多极扩展方案中的单极截断。单体。这项工作中引入的变分X-Pol电势的公式(我们称为“多极变分X-Pol电势”)代表了其波函数以与变函数相同的方式进行变分优化的单体的电子密度。代表计算外部单体之间的库仑相互作用时外部单体的电子密度。

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