Deexcitation and recombination of excited ions involving doubly excited states in dense recombining plasma: Lithiumlike ion x-ray laser

1996 ◽  
Author(s):  
Takashi Fujimoto ◽  
Tetsuya Kawachi
2002 ◽  
Vol 80 (8) ◽  
pp. 821-835 ◽  
Author(s):  
H Tawara ◽  
P Richard ◽  
U I Safronova ◽  
A A Vasilyev ◽  
M Stockli

M X-rays have been observed from 1–40 keV/u 181Taq+ (q = 45–49) ions colliding with neutral Ar atoms under single collisions. The most dominant X-rays have been found to be due to transitions of 4p–3d and 4f–3d when the projectiles bring 3d-shell vacancies into collisions. Though much weaker, M X-rays also have been observed in collisions with Ta45+ ions that initially have no 3d-shell vacancy and are understood to originate from transitions of the doubly excited states 3d9nln'l' formed through strong electron–electron interactions after single-electron capture. The observed M X-ray spectra have been compared and reproduced nicely with the synthesized spectra. It has been confirmed that transitions of such doubly excited states also contribute to X-rays at the lower energy region observed even for higher charge ions with 3d vacancies. PACS Nos.: 32.30Rj, 32.70Cs, 32.80Rm, 34.70+e


2021 ◽  
Vol 9 ◽  
Author(s):  
Bo Han ◽  
Feilu Wang ◽  
David Salzmann ◽  
Jiayong Zhong ◽  
Gang Zhao

Abstract In this paper, we present a reanalysis of the silicon He- $\mathrm{\alpha}$ X-ray spectrum emission in Fujioka et al.’s 2009 photoionization experiment. The computations were performed with our radiative-collisional code, RCF. The central ingredients of our computations are accurate atomic data, inclusion of satellite lines from doubly excited states and accounting for the reabsorption of the emitted photons on their way to the spectrometer. With all these elements included, the simulated spectrum turns out to be in good agreement with the experimental spectrum.


2000 ◽  
Vol 85 (26) ◽  
pp. 5559-5562 ◽  
Author(s):  
R. Schuch ◽  
S. Madzunkov ◽  
E. Lindroth ◽  
D. Fry

2009 ◽  
Vol 102 (15) ◽  
Author(s):  
M. Alagia ◽  
M. Coreno ◽  
H. Farrokhpour ◽  
P. Franceschi ◽  
A. Mihelič ◽  
...  

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