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An ab-initio many-body method for electronic structure calculations of solids. I. Description of the method

机译:一种用于电子结构计算的ab-initio多体方法   固体。 I.方法的描述

摘要

We propose a new, alternative method for ab-initio calculations of theelectronic structure of solids, which has been specifically adapted to treatmany-body effects in a more rigorous way than many existing ab-initio methods.We start from a standard band-structure calculation for an effectiveone-particle Hamiltonian approximately describing the material of interest.This yields a suitable set of one-particle basis functions, from which welllocalized Wannier functions can be constructed using a method proposed byMarzari and Vanderbilt. Within this (minimal) basis of localized Wannierfunctions the matrix elements of the non-interacting (one-particle) Hamiltonianas well as the Coulomb matrix elements can be calculated. The result is amany-body Hamiltonian in second quantization with parameters determined fromfirst principles calculations for the material of interest. The Hamiltonian isin the form of a multi-band Hamiltonian in second quantization (a kind ofextended, multi-band Hubbard model) such that all the standard many-bodymethods can be applied. We explicitly show how this approach can be solved inthe simplest many-body approximation, the mean-field Hartree-Fock approximation(HFA), which takes into account exact exchange and corrects forself-interaction effects.
机译:我们提出了一种用于固体电子结构的从头算式的新方法,该方法比许多现有的从头算式方法更严格地专门用于处理多体效应。我们从标准的带结构计算开始一个有效的单粒子哈密顿量近似描述了感兴趣的物质。这产生了一组合适的单粒子基函数,可以使用Marzari和Vanderbilt提出的方法来构造定位良好的Wannier函数。在局部万尼尔函数的这个(最小)基础上,可以计算出非相互作用(单粒子)哈密顿氏菌的矩阵元素以及库仑矩阵元素。结果是第二次量化中的多体哈密顿量,其参数是从感兴趣材料的第一原理计算中确定的。哈密​​顿量在第二量化中是多频带哈密顿量的形式(一种扩展的多频带哈伯德模型)​​,因此可以应用所有标准的多体方法。我们明确显示了如何通过最简单的多体近似(均场Hartree-Fock近似(HFA))解决该方法,该方法考虑了精确的交换并校正了自身交互作用。

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