Differential inverse inelastic mean free path determination on the base of X-ray photoelectron emission spectra

Author(s):  
V. P. Afanas’ev ◽  
A. S. Gryazev ◽  
D. S. Efremenko ◽  
P. S. Kaplya ◽  
N. V. Lyapunov
1997 ◽  
Vol 13 (5) ◽  
pp. 797-801 ◽  
Author(s):  
Jun KAWAI ◽  
Hirohiko ADACHI ◽  
Yoshinori KITAJIMA ◽  
Kuniko MAEDA ◽  
Shinjiro HAYAKAWA ◽  
...  

1991 ◽  
Vol 35 (B) ◽  
pp. 857-867
Author(s):  
M.F. Ebel ◽  
H. Ebel ◽  
F. Olcaytug

The depth range d of x-ray photoelectron spectrometry (XPS) is determined by the inelastic mean free path λ of photoelectrons . The following considerations are dedicated to a correlation between d and λ.


1993 ◽  
Vol 3 (7) ◽  
pp. 1649-1659
Author(s):  
Mohammad A. Tafreshi ◽  
Stefan Csillag ◽  
Zou Wei Yuan ◽  
Christian Bohm ◽  
Elisabeth Lefèvre ◽  
...  

2021 ◽  
Vol 118 (5) ◽  
pp. 053104
Author(s):  
L. H. Yang ◽  
B. Da ◽  
H. Yoshikawa ◽  
S. Tanuma ◽  
J. Hu ◽  
...  

Vacuum ◽  
1983 ◽  
Vol 33 (10-12) ◽  
pp. 767-769 ◽  
Author(s):  
V.M. Dwyer ◽  
J.A.D. Matthew

2000 ◽  
Vol 6 (S2) ◽  
pp. 224-225
Author(s):  
A. Aitouchen ◽  
T. Chou ◽  
M. Libera ◽  
M. Misra

The common experimental method to determine the total inelastic mean free path i by electron energy-loss spectroscopy (EELS) is by the relation : t/λi= ln(It/IO) [1] where t is the specimen thickness, It, is the total integrated intensity, and Io is the intensity of the zero-loss peak. The accuracy of this measurement depends on the thickness determination. Model geometries like cubes, wedges, and spheres enable accurate thickness determination from transmission images.Spherical polymers with diameters of order 10-200nm can be made from a number of high-Tg polymers by solvent atomization. This research studied atomized spheres of poly(2-vinyl pyridine) [PVP]. A solution of 0.1% PVP in THF was nebulized. After solvent evaporation during free fall within the chamber atmosphere, solid spherical polymer particles with a range of diameters were collected on holey-carbon TEM grids at the bottom of the atomization chamber.


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