Electron scattering cross section calculations for polar molecules over a broad energy range

2014 ◽  
Vol 83 ◽  
pp. 57-67 ◽  
Author(s):  
A.G. Sanz ◽  
M.C. Fuss ◽  
F. Blanco ◽  
Zdeněk Mašín ◽  
Jimena D. Gorfinkiel ◽  
...  
Keyword(s):  
Energy Range ◽  
Cross Section ◽  
Electron Scattering ◽  
Scattering Cross Section ◽  
Polar Molecules ◽  
Scattering Cross ◽  
Broad Energy Range ◽  
Broad Energy

Electron scattering cross sections from anthracene over a broad energy range (0.00001–10,000eV)

2014 ◽  
Vol 83 ◽  
pp. 68-76 ◽  
Author(s):  
A.G. Sanz ◽  
M.C. Fuss ◽  
F. Blanco ◽  
F. Carelli ◽  
F. Sebastianelli ◽  
...  
Keyword(s):  
Energy Range ◽  
Electron Scattering ◽  
Cross Sections ◽  
Scattering Cross ◽  
Broad Energy Range ◽  
Scattering Cross Sections ◽  
Broad Energy

scholarly journals Total electron scattering cross section from pyridine molecules in the energy range 10–1000 eV

2018 ◽  
Vol 699 ◽  
pp. 182-187 ◽  
Author(s):  
A. Traoré Dubuis ◽  
F. Costa ◽  
F. Ferreira da Silva ◽  
P. Limão-Vieira ◽  
J.C. Oller ◽  
...  
Keyword(s):  
Energy Range ◽  
Cross Section ◽  
Electron Scattering ◽  
Scattering Cross Section ◽  
Total Electron ◽  
Scattering Cross

Mass Determination by Direct Measurement of Electron Scattering

1975 ◽  
Vol 33 ◽  
pp. 240-241
Author(s):  
M. K. Lamvik ◽  
A. V. Crewe
Keyword(s):  
Cross Section ◽  
Electron Scattering ◽  
Mass Density ◽  
Variable Mass ◽  
Scattering Cross Section ◽  
Mass Determination ◽  
Number Density ◽  
Cross Sectional ◽  
Thin Slice ◽  
Scattering Cross

If a molecule or atom of material has molecular weight A, the number density of such units is given by n=Nρ/A, where N is Avogadro's number and ρ is the mass density of the material. The amount of scattering from each unit can be written by assigning an imaginary cross-sectional area σ to each unit. If the current I0 is incident on a thin slice of material of thickness z and the current I remains unscattered, then the scattering cross-section σ is defined by I=IOnσz. For a specimen that is not thin, the definition must be applied to each imaginary thin slice and the result I/I0 =exp(-nσz) is obtained by integrating over the whole thickness. It is useful to separate the variable mass-thickness w=ρz from the other factors to yield I/I0 =exp(-sw), where s=Nσ/A is the scattering cross-section per unit mass.

Electron Scattering Cross Section on the Surface of Thin Ag and Au Films Induced by Atomic Deuterium Adsorption

Langmuir ◽  
2004 ◽  
Vol 20 (21) ◽  
pp. 9138-9143 ◽  
Author(s):  
Ryszard Duś ◽  
Ewa Nowicka ◽  
Robert Nowakowski
Keyword(s):  
Cross Section ◽  
Electron Scattering ◽  
Scattering Cross Section ◽  
Scattering Cross

scholarly journals Factor analysis of inelastic electron scattering cross section spectra of FeSi2

2019 ◽  
Vol 467 ◽  
pp. 012010
Author(s):  
A. Yu. Igumenov ◽  
A. S. Parshin ◽  
V. O. Kanzychakova ◽  
A. M. Demin ◽  
T. A. Andryushchenko ◽  
...  
Keyword(s):  
Factor Analysis ◽  
Cross Section ◽  
Electron Scattering ◽  
Scattering Cross Section ◽  
Inelastic Electron ◽  
Scattering Cross ◽  
Inelastic Electron Scattering
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