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Expressions of energy and potential due to orbital polarization

机译:轨道极化引起的能量和势的表达

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摘要

The simple and tractable representation for the LS-multiplet energy in l(1)l(2)-configuration in an atom is derived in the form of the polynomials being a function Of l(1) (.) l(2) Which obey the recurrence formulae, and is suitable for the vector model. Moreover, it is extended to P configurations. On a basis of the model, the definition of the orbital polarization energy is given. The more precise expressions of the energies compared to those so far proposed by Eriksson et al. are derived for the maximal spin multiplets in p(n), d(n), and f(n). They are composed of two terms depending on -3L(2)/2 and n(n - 2l - 1). They are the exact for p(n) and d(n), but it for f(n) is correct only for a ground multiplet. Other expressions are also derived as a function of L 2 for f(n), though more complicated. For the actual atomic and band structure calculations based on local-spin-density-approximation (LSDA), the modified expression for the energy is proposed. The potential is derived from its expression in terms of the density functional theory, and can be applied to their Structure calculations.
机译:原子中l(1)l(2)-构型中LS多重能量的简单易处理表示形式是服从l(1)(。)l(2)的函数的多项式形式递推公式,适用于向量模型。此外,它扩展为P配置。在此模型的基础上,给出了轨道极化能的定义。与迄今为止Eriksson等人提出的能量相比,能量的表达更为精确。推导p(n),d(n)和f(n)中的最大自旋多重峰。它们由取决于-3L(2)/ 2和n(n-2l-1)的两个项组成。它们对于p(n)和d(n)是精确的,但对于f(n)则仅对于地面多重峰是正确的。其他表达式也可以作为f(n)的L 2的函数导出,尽管更为复杂。对于基于局部自旋密度近似(LSDA)的实际原子和能带结构计算,提出了能量的修正表达式。势是根据密度泛函理论从其表达式得出的,可以应用于其结构计算。

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