scholarly journals Irradiated fuel monitoring by Cerenkov glow intensity measurements

1979 ◽  
Author(s):  
E.J. Dowdy ◽  
N. Nicholson ◽  
J.T. Caldwell

Author(s):  
M.D. Ball ◽  
H. Lagace ◽  
M.C. Thornton

The backscattered electron coefficient η for transmission electron microscope specimens depends on both the atomic number Z and the thickness t. Hence for specimens of known atomic number, the thickness can be determined from backscattered electron coefficient measurements. This work describes a simple and convenient method of estimating the thickness and the corrected composition of areas of uncertain atomic number by combining x-ray microanalysis and backscattered electron intensity measurements.The method is best described in terms of the flow chart shown In Figure 1. Having selected a feature of interest, x-ray microanalysis data is recorded and used to estimate the composition. At this stage thickness corrections for absorption and fluorescence are not performed.



2011 ◽  
pp. 107-114
Author(s):  
B. Lacroix ◽  
T. Martella ◽  
M. Pras ◽  
M. Masson-Fauchier ◽  
L. Fayette


2008 ◽  
Author(s):  
Christian Deck ◽  
Chinung Ni ◽  
Kenneth Vecchio ◽  
Prabhakar Bandaru


2020 ◽  
Vol 145 ◽  
pp. 107515
Author(s):  
Sangang Li ◽  
Zhengyun Dong ◽  
Quan Gan ◽  
Jing Song ◽  
Qi Yang




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