Calculations of 5dN-16s systems using orthogonal operators: do orthogonal operators survive configuration interaction?

P. Uylings, A. Raassen, J. Wyart
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引用次数: 30

Abstract

The merits and pitfalls of using orthogonal operators in systems with strong configuration interaction are illustrated by a study of a number of (5d+6s)N configurations (N=8, 9) ranging from Ir to Pb. Both the perturbational and the full diagonalization approach are applied. Criteria are given to indicate the regions where either operators based on perturbation theory or explicit configuration interactions are dominant. In both regions, orthogonal operators describe the (ground and) excited states well, provided they are extended by interconfiguration operators in the case of lower ionization, where full diagonalization of the three (5d+6s)N configurations is required. Ab initio calculations using second order perturbation theory show satisfactory agreement with the results from fits to experimental energy levels, except again for the lowest ionizations, where perturbation theory breaks down. It turns out to be a good approximation to exclude interactions treated by complete diagonalization from the perturbation expressions; both approaches can then be combined to describe excited state interactions.
5dN-16s系统的正交算符计算:正交算符能在组态交互中存活吗?
通过对Ir ~ Pb范围内的(5d+6s)N组态(N= 8,9)的研究,说明了在具有强组态相互作用的系统中使用正交算子的优点和缺陷。采用了微扰法和完全对角化法。给出了表明基于微扰理论或显式组态相互作用的算子占主导地位的区域的准则。在这两个区域中,正交算符都能很好地描述(基态和)激发态,只要它们在低电离的情况下被组态间算符扩展,在低电离的情况下,需要三个(5d+6s)N组态的完全对角化。使用二阶微扰理论的从头计算与实验能级的拟合结果一致,除了最低的电离,在那里微扰理论失效。从摄动表达式中排除完全对角化处理的相互作用是一个很好的近似;这两种方法可以结合起来描述激发态相互作用。
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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