2013
DOI: 10.1088/0031-8949/87/03/035302
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The second spectrum of niobium: I. Accurate fine structure study of even-parity levels

Abstract: For the first time, a parametric analysis of the fine and hyperfine structure for even-parity levels of Nb II, involving 17 configurations, has been performed. The interpretation has been carried out based on a linked-parameter method of level-fitting calculations in a large multiconfiguration basis. The sets of fine structure parameters, the leading eigenvector percentages of levels, as well as their calculated magnetic Landé g-factors are newly given. Furthermore, we confirm on the whole the validity of the … Show more

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Cited by 6 publications
(6 citation statements)
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“…Our computed HFS data confirm totally, as in the case of even-parity levels [24], the experimental data of Nilson and Ivarson [17], even those given this time with the biggest relative uncertainty, i.e. 4%, and also those of Young et al [16] and Cheal et al [18], which are very accurate.…”
Section: Accurate Fine and Hyperfine Structure Analysessupporting
confidence: 87%
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“…Our computed HFS data confirm totally, as in the case of even-parity levels [24], the experimental data of Nilson and Ivarson [17], even those given this time with the biggest relative uncertainty, i.e. 4%, and also those of Young et al [16] and Cheal et al [18], which are very accurate.…”
Section: Accurate Fine and Hyperfine Structure Analysessupporting
confidence: 87%
“…Moreover, we have pointed out in a previous work [6] that for many elements the ratio F K , between F=a 10 ns (n − 1) d 2 nsnp exp /a 10 ns (n − 1) d 3 ns exp and K = a 10 ns (n − 1) d 2 nsnp cal /a 10 ns (n − 1) d 3 ns cal , is the same within uncertainties and is equal to 1.169 (average value). Assuming that polarizing effects remain the same whatever the number of p-electrons [19,25,26] and using a 10 5s 4d 3 5s 1 exp = 272.06 mK [24], one obtains by the simple rule of three: Finally, one can see good agreement between fitted HFS one-electron radial parameters and the calculated ones, gathered in table 4 for d-electrons, p-electrons and even for s-electrons, reinforcing once more the reliability of the model used for fitting.…”
Section: Accurate Fine and Hyperfine Structure Analysesmentioning
confidence: 99%
“…We confirm on the whole the attributions to term designations given previously [1]- [3] We propose to invert these two triplet positions as we did in Table 1. It has been brought immediately to our attention by experimental hfs data given in for the 3d 3 4s configuration obtained thanks to the fs study and ab initio calculations, as we did previously [4]- [8]. In Table 4 we give up to 100,000 cm −1 our predicted data for missing experimental energies for these five configurations, analysed in [1]- [3].…”
Section: Accurate Fine and Hyperfine Structure Analysismentioning
confidence: 77%
“…The interactions between particular states are determined quantitatively by this analysis. The complete details of fs analysis were already given in our previous papers: see for instance [8].…”
Section: Accurate Fine and Hyperfine Structure Analysismentioning
confidence: 99%
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