Self-consistent Field Orbital Methods

J. Autschbach
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Abstract

This chapter discusses the concepts underlying the Hartree-Fock (HF) electronic structure method. First, it is shown how the energy expectation value is calculated for a Slater determinant (SD) wavefunction in the case of orthonormal orbitals. This leads to the definition of the electron repulsion integrals (ERIs). Next, the energy is minimized subject to the orthonormality constraints. This leads to the HF equation for the orbitals. The HF orbital energies are Langrange multipliers representing the constraints. An unknown set of orbitals can be determined from an initial guess via a self-consistent field (SCF) cycle. The HF scheme is discussed for closed-shell versus open shell systems, leading to the distinction between spin restricted and unrestricted HF (RHF, UHF). Kohn-Sham density functional theory (DFT) is introduced and its approximate version is placed in the context of ab-initio versus semi-empirical quantum chemistry methods.
自洽场轨道法
本章讨论了Hartree-Fock (HF)电子结构方法的基本概念。首先,它显示了在标准正交轨道的情况下如何计算斯莱特行列式(SD)波函数的能量期望值。这导致了电子排斥积分(ERIs)的定义。其次,根据正交性约束最小化能量。这就引出了轨道的HF方程。HF轨道能量是表示约束条件的朗朗日乘子。一组未知的轨道可以通过自洽场循环从初始猜测中确定出来。讨论了闭壳和开壳体系的高频格式,从而区分了自旋受限HF和不受限制HF (RHF, UHF)。介绍了Kohn-Sham密度泛函理论(DFT),并将其近似版本置于从头算与半经验量子化学方法的背景下。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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