2017
DOI: 10.1139/cjp-2016-0746
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Overview of recent advances performed in the study of atomic structures and radiative processes for the lowest ionization stages of heavy elements

Abstract: During the past 20 years, part of our work has been focused on the study of the atomic structure and the determination of radiative parameters in neutral and slightly ionized heavy atoms (Z ≥ 37). These elements attracted little previous interest because of the complexity of their electronic structures, the poor knowledge of their spectra, and the difficulty to perform experimental measurements. They present, however, great interest in the development of other scientific areas, such as astrophysics and plasma … Show more

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Cited by 18 publications
(12 citation statements)
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“…However, as in the case of our previous analysis related to Er III, such core-polarization corrections were not considered in the atomic orbital calculation of the ground configuration 4f 12 . The 4f electrons being indeed located deep inside the Xe-like 5s 2 5p 6 ionic core, the analytical polarization corrections to the dipole operator as introduced in our model [25][26][27] are no longer valid for transitions involving these electrons. As an alternative, the uncorrected <4f|r|5d> radial matrix element corresponding to the 4f 12 -4f 11 5d transitions was scaled down by a factor 0.81, as we proceeded for Er III [24].…”
Section: Computational Methods Usedmentioning
confidence: 87%
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“…However, as in the case of our previous analysis related to Er III, such core-polarization corrections were not considered in the atomic orbital calculation of the ground configuration 4f 12 . The 4f electrons being indeed located deep inside the Xe-like 5s 2 5p 6 ionic core, the analytical polarization corrections to the dipole operator as introduced in our model [25][26][27] are no longer valid for transitions involving these electrons. As an alternative, the uncorrected <4f|r|5d> radial matrix element corresponding to the 4f 12 -4f 11 5d transitions was scaled down by a factor 0.81, as we proceeded for Er III [24].…”
Section: Computational Methods Usedmentioning
confidence: 87%
“…More precisely, the configuration sets explicitly retained for the computations were 4f 12 , 4f 11 6p, 4f 11 7p, 4f 11 5f, 4f 11 6f for the even parity, and 4f 11 6s, 4f 11 7s, 4f 11 5d, 4f 11 6d, 4f 11 7d for the odd parity. The core-valence interactions were included by means of a core-polarization pseudo-potential and a correction to the dipole operator according to the procedure described in many of our previous papers (see e.g., [25][26][27]). As a reminder, for atomic systems with n valence electrons, this core-polarization potential gives rise to the following one-particle, V P1 , and two-particle, V P2 , contributions:…”
Section: Computational Methods Usedmentioning
confidence: 99%
“…It is worth noting however that, three of these Comparison between experimental and theoretical strongest emission lines in U II. Only visible spectral lines observed by Palmer et al (1980) with measured intensities greater than 10 (top figure) and those calculated in this work with weighted transition probabilities, gA, larger than 10 7 s −1 (bottom figure) are shown.…”
Section: R E S U Lt S a N D Discussionmentioning
confidence: 97%
“…In their critical compilation related to actinides, Blaise & Wyart (1992) listed some preliminary U II energy levels, using the emission lines listed by Steinhaus et al (1971) and Palmer, Keller & Engleman (1980), thus updating the previous estimates published by Brewer (1971). An uranium hollow-cathode Fourier transform spectrum between 1800 and 42 000cm −1 was then combined with previous visible and ultraviolet spectra by Blaise et al (1994) who were able to determine the numerical values for 354 and 809 energy levels belonging to the four odd configurations 5f 3 7s 2 , 5f 3 6d7s, 5f 3 6d 2 , 5f 4 7p, and to the six even configurations 5f 4 7s, 5f 4 6d, 5f 2 6d 2 7s, 5f 2 6d7s 2 , 5f 3 7s7p, 5f 3 6d7p, respectively.…”
Section: Ava I L a B L E Ato M I C Data I N U Iimentioning
confidence: 99%
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