Experimental cross sections for two-electron capture into nitrogen autoionising states in Nq+ (q = 6, 7) on He and H2 collisions at 10.5q keV

Author(s):  
A. Bordenave-Montesquieu ◽  
P. Benoit-Cattin ◽  
A. Gleizes ◽  
A.I. Marrakchi ◽  
S. Dousson ◽  
...  
1984 ◽  
Vol 29 (5) ◽  
pp. 2457-2462 ◽  
Author(s):  
W. Waggoner ◽  
C. L. Cocke ◽  
S. L. Varghese ◽  
M. Stockli

1996 ◽  
Vol 53 (4) ◽  
pp. 2337-2344 ◽  
Author(s):  
J.-Y. Chesnel ◽  
H. Merabet ◽  
X. Husson ◽  
F. Frémont ◽  
D. Lecler ◽  
...  

2009 ◽  
Vol 80 (4) ◽  
Author(s):  
M. M. Sant’Anna ◽  
A. C. F. Santos ◽  
L. F. S. Coelho ◽  
Ginette Jalbert ◽  
N. V. de Castro Faria ◽  
...  

1996 ◽  
Vol 74 (5-6) ◽  
pp. 230-235 ◽  
Author(s):  
D. V. Rao ◽  
R. Cesareo ◽  
G. E. Gigante

LL, Lα, Lβ, and Lγ X-ray fluorescence cross sections for Pr, Sm, Gd, Dy, Ho, Er, Yb, Pt Au, and Pb were measured at the excitation energy 16.58 keV. An X-ray tube and a secondary excitor system was used instead of radioisotopes for the measurements. Experimental cross sections are compared with the theoretical estimates based on relativistic Dirac–Hartree–Slater theory. Average L-shell fluorescence yields [Formula: see text] are deduced using the present experimental cross sections and the theoretical subshell photoionization cross sections. The derived average fluorescence yields are fitted by least squares to polynomials in Z of the form ΣnanZn and compared with theoretical and earlier fitted values. Good agreement is observed ' between the experimental results and the theoretical estimates based on relativistic Dirac–Hartree–Slater theory.


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