Dielectronic recombination and satellite line spectra of highly charged tungsten ions

被引:9
|
作者
Safronova, U. I. [1 ]
Safronova, A. S. [1 ]
Beiersdorfer, P. [2 ]
机构
[1] Univ Nevada, Dept Phys, Reno, NV 89557 USA
[2] Lawrence Livermore Natl Lab, Div Phys, Livermore, CA 94550 USA
关键词
MANY-BODY CALCULATIONS; TRANSITION-PROBABILITIES; X-RAY; RATE COEFFICIENTS; EXCITED-STATES; NI; WAVELENGTHS; RATES; ENERGIES; BARIUM;
D O I
10.1139/P10-114
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
We present our recent progress on theoretical studies that involve auto-ionizing states of highly charged tungsten ions. Such auto-ionizing states have two channels for decay, which requires that both radiative and auto-ionization atomic data be calculated and combined in a detailed study of the dielectronic recombination (DR). Three atomic codes are used to produce relativistic atomic data (energy levels, radiative transition probabilities, and auto-ionization rates). These are the relativistic many-body perturbation theory (RMBPT) code, the multiconfiguration relativistic Hebrew University Lawrence Livermore atomic code (HULLAC), and the Hartree-Fock relativistic (Cowan) code. Branching ratios relative to the first threshold and intensity factors are calculated for satellite lines, and DR rate coefficients are determined for the excited states. The total DR rate coefficient is derived as a function of electron temperature, and it is shown that the contribution of the highly excited states is very important for the calculation of the total DR rates. Synthetic dielectronic satellite spectra are constructed, and the atomic properties specific to the relevant tungsten ions are highlighted. First, we will consider the results for Na-like tungsten (W63+) and Mg-like tungsten (W62+) using all three codes. Then, we move to even higher ionization states and present the results in Li-like W (W71+). For this we use the RMBPT code as well as the quasi-relativistic many-body perturbation theory (MZ) code. The inclusion of the DR process is essential for correct identification of the lines in impurity spectra and for understanding the main contributions to the total radiation losses.
引用
收藏
页码:581 / 589
页数:9
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