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Analysis of self-consistency effects in range-separated density-functional theory with M?sller-Plesset perturbation theory

机译:用M?sller-Plesset摄动理论分析距离分隔密度泛函理论中的自洽效应

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Range-separated density-functional theory combines wave function theory for the long-range part of the two-electron interaction with density-functional theory for the short-range part. When describing the long-range interaction with non-variational methods, such as perturbation or coupled-cluster theories, self-consistency effects are introduced in the density functional part, which for an exact solution requires iterations. They are generally assumed to be small but no detailed study has been performed so far. Here, the authors analyze self-consistency when using Mller-Plesset-type (MP) perturbation theory for the long range interaction. The lowest-order self-consistency corrections to the wave function and the energy, that enter the perturbation expansions at the second and fourth order, respectively, are both expressed in terms of the one-electron reduced density matrix. The computational implementation of the latter is based on a Neumann series which, interestingly, even though the effect is small, usually diverges. A convergence technique, which perhaps can be applied in other uses of Neumann series in perturbation theory, is proposed. The numerical results thus obtained show that, in weakly bound systems, self-consistency can be neglected since the long-range correlation does not affect the density significantly. Although MP is not adequate for multireference systems, it can still be used as a reliable analysis tool. Though the density change is not negligible anymore in such cases, self-consistency effects are found to be much smaller than long-range correlation effects (less than 10 for the systems considered). For that reason, a sensible approximation might be to update the short-range energy functional term while freezing its functional derivative, namely, the short-range local potential, in the wave function optimization. The accuracy of such an approximation still needs to be assessed.
机译:距离分离的密度泛函理论将波函数理论用于两电子相互作用的远距离部分,并将密度泛函理论用于短距离部分。当描述与非变分方法(例如微扰或耦合聚类理论)的远程交互时,密度函数部分引入了自洽效应,要获得精确的解决方案,需要进行迭代。通常认为它们很小,但是到目前为止尚未进行详细的研究。在这里,作者分析了使用Mller-Plesset型(MP)扰动理论进行远程交互时的自洽性。对波函数和能量的最低阶自洽校正(分别以二阶和四阶输入扰动扩展)均以单电子降密度矩阵表示。后者的计算实现基于Neumann级数,有趣的是,尽管效果很小,但通常会发散。提出了一种收敛技术,也许可以将它应用于微扰理论中的诺伊曼级数的其他用途。如此获得的数值结果表明,在弱约束系统中,由于长期相关不会显着影响密度,因此可以忽略自洽。尽管MP不足以用于多参考系统,但它仍可以用作可靠的分析工具。尽管在这种情况下密度变化不再可以忽略不计,但发现自洽效应远小于远程相关效应(对于所考虑的系统,其小于10)。因此,在波动函数优化中,合理的近似方法可能是更新短程能量函数项,同时冻结其函数导数,即短程局部电势。仍然需要评估这种近似的准确性。

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