Electronic properties of vanadium pentoxide by inelastic scattering method

2021 ◽  
Author(s):  
Gunjan Arora ◽  
Pooja K. Joshi ◽  
Kishor Kumar ◽  
B. L. Ahuja

Physica ◽  
1967 ◽  
Vol 35 (4) ◽  
pp. 441-450 ◽  
Author(s):  
W. Jakób ◽  
J.M. Janik ◽  
J.A. Janik ◽  
A. Bajorek ◽  
K. Parliński ◽  
...  


Physica ◽  
1967 ◽  
Vol 35 (4) ◽  
pp. 457-464 ◽  
Author(s):  
J.M. Janik ◽  
J.A. Janik ◽  
A. Bajorek ◽  
K. Parliński ◽  
M. Sudnik-Hrynkiewicz


1992 ◽  
pp. 515-520
Author(s):  
J.C. Badot ◽  
D. Gourier ◽  
N. Baffier ◽  
R. Morineau


Physica ◽  
1967 ◽  
Vol 35 (4) ◽  
pp. 465-468 ◽  
Author(s):  
A. Bajorek ◽  
K. Parliński ◽  
M. Sudnik-Hrynkiewicz


Physica ◽  
1967 ◽  
Vol 35 (4) ◽  
pp. 451-456 ◽  
Author(s):  
J.A. Janik ◽  
J.M. Janik ◽  
A. Bajorek ◽  
K. Parliński ◽  
M. Sudnik-Hrynkiewicz




Physica ◽  
1967 ◽  
Vol 35 (4) ◽  
pp. 469-474 ◽  
Author(s):  
A. Bajorek ◽  
K. Parliński ◽  
M. Sudnik-Hrynkiewicz ◽  
J.A. Janik


Author(s):  
S. Golladay

The theory of multiple scattering has been worked out by Groves and comparisons have been made between predicted and observed signals for thick specimens observed in a STEM under conditions where phase contrast effects are unimportant. Independent measurements of the collection efficiencies of the two STEM detectors, calculations of the ratio σe/σi = R, where σe, σi are the total cross sections for elastic and inelastic scattering respectively, and a model of the unknown mass distribution are needed for these comparisons. In this paper an extension of this work will be described which allows the determination of the required efficiencies, R, and the unknown mass distribution from the data without additional measurements or models. Essential to the analysis is the fact that in a STEM two or more signal measurements can be made simultaneously at each image point.



Sign in / Sign up

Export Citation Format

Share Document