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中国物理学会期刊

Rh XIII—Cd XVI离子4s24p3—4s4p4能级与跃迁的理论计算

CSTR: 32037.14.aps.68.20181976

Theoretical study of energy levels and transitions 4s24p3−4s4p4 for ions Rh XIII to Cd XVI

CSTR: 32037.14.aps.68.20181976
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  • 用HFR (Hartree-Fock with relativistic corrections)方法对Rb V—Cd XVI离子4s24p3和4s4p4组态能级结构做了全面系统的理论计算研究. 通过分析能级结构参数的HFR理论计算值与基于实验能级拟合得到的计算值之比值随着原子序数Zc变化的规律, 运用广义拟合外推方法预言了这些离子能级结构参数. 由此进一步计算了Rh XIII, Pd XIV, Ag XV和Cd XVI离子4s24p3 (4S3/2, 2P1/2, 3/2, 2D3/2, 5/2)和4s4p4 (4P1/2, 3/2, 5/2, 2P1/2, 3/2, 2D3/2, 5/2, 2S1/2)组态能级以及电偶极跃迁波长与振子强度. 研究表明, 对于4s24p3组态, 单组态近似可以得到较满意的结果; 而对于4s4p4组态, 只有在考虑了4s24p24d的组态相互作用效应时, 计算结果的准确性才能明显得到提高. 同时, 本文还运用全相对论grasp2K-DEV程序包计算了Rh XIII—Cd XVI离子组态能级. 对于Rh XIII离子4s24p3 (2P1/2), Pd XIV离子4s24p3 (4S3/2, 2P1/2, 3/2, 2D3/2, 5/2)和4s4p4 (2P1/2, 3/2, 2D3/2, 5/2, 2S1/2), 能级均无实验值; 对于Ag XV和Cd XVI离子, 截至目前还没实验能级数据, 没有实验能级值的所有数据均仅来自本文的计算数值. 本文计算结果与已有实验值吻合得很好.

     

    Ions from Rh XIII to Cd XVI belong to the arsenic isoelectronic sequence ions. Their ground configuration is 4s24p3, and the lower excited configurations are 4s4p4, 4s24p24d and 4s24p25s etc. The present study aims to predict the energy levels and transition data unknown in experiment for configurations 4s24p3 and 4s4p4 from Rh XIII to Cd XVI ions, by analyzing the trend of the variation of Slater-Condon parameters along the As-like sequence based on the experimental energy levels available in the literature. So, the theoretical analyses of fine-structure energy levels of these configurations are conducted for the sequence ions from Rb V to Cd XVI by Hartree-Fock with Relativistic correction (HFR) method in Cowan’ code. The Slater-Condon parameter values of energy levels are obtained by least-square-fit (LSF) technique for ions mentioned above with the available experimental data. For the unknown parameters, the generalized-least-square-fit (GLSF) technique is used together with the extra (or inter)-polation method. With these new parameter values, the energy levels of 4s24p3 and 4s4p4, the wavelengths and oscillator strengths of the transition array 4s24p3−4s4p4 are computed. This research shows that for 4s24p3, the single-configuration approximation of HFR calculation can present the satisfactory results, however, for 4s4p4, the reasonable good results can be achieved only by multi-configuration(4s4p4 + 4s24p24d) approximation, which can be verified by the obtained data. Comparing the absolute differences between observed and present LSF calculated levels’ values (including multi-configuration interaction) for the 4s4p4 configuration in ions from Rb V to Mo X with the results computed in a similar Hartree-Fock single-configuration approximate method by Person and Pettersson (Person W, Pettersson S G 1984 Phys. Scr. 29 308), we can see that the present LSF energy levels are improved substantially. For example, the LSF minimum and maximum absolute deviation value at present are 1 cm–1 and 140 cm–1, respectively, much more accurate than the results presented by Person et al., which are 45 cm–1 and 382 cm–1. The predicted data are in good agreement with the experimental results. For obtaining more information, the energy levels of 4s24p3 and 4s4p4 configurations are computed by grasp2K-DEV package in valence-valence correlation scheme, which is based on the fully relativistic multi-configuration Dirac-Hartree-Fock (MCDHF) theory. The overall MCDHF energy levels are generally in accordance with the experimental results. The data obtained in this research are expected to be used in the future relevant theoretical and experimental investigations.

     

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