Abstract

The hyperfine and Zeeman structures of 14 lines of isotope 123Sb covering the UV-NIR spectral range have been measured. The experimental data have been used in order to reanalyse and revise Sb I energy levels. We named majority of them for the first time since they were previously labelled only by their energy values, without any term designations. In both cases of odd- and even-parity levels we took into consideration up to 7 interacting configurations; the set of fine structure parameters and the leading eigenvector percentages of levels as well as their calculated Lande-factors are given. Semi-empirical hfs parameter values extracted from experimental data were compared with ab initio results computed by the use of Cowan code.

Highlights

  • Natural antimony consists of two stable isotopes 121Sb (I = 5/2) and 123Sb (I = 7/2), with natural abundance of 57% and 43%, respectively

  • Semi-empirical hfs parameter values extracted from experimental data were compared with ab initio results computed by the use of Cowan code

  • The experimental energy levels, calculated eigenvalues, resulting LS-percentage of first and second components of the wave functions, and the corresponding LS-term designations are given. In this table our experimental Lande gJ -factors, as well as those found in literature are compared to those deduced from the eigenvector compositions and those computed by ab initio procedure, recurring to Cowan code [37]

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Summary

Introduction

Hyperfine structure splitting A and B constants for levels of the ground configuration of Sb I have been obtained in a number of experiments [3,4,5,6,7,8,9,10,11]. At the beginning of Sb I electronic structure studies, looked into the emission spectrum. In paper [5] the hfs of forbidden lines between levels belonging to the ground configuration of Sb I was studied. In this paper we report results of observation of hfs and Zeeman structure of 14 emission lines of 123Sb I covering the UV-NIR spectral range (363.8÷1074.2) nm

Experiment
Experimental results
Fine structure considerations for odd-parity levels
Fine structure considerations for even-parity levels
Hyperfine interaction
Hyperfine structure considerations for odd-parity levels
Hyperfine structure considerations for even-parity levels
Conclusion

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