The effect of the relativistic Hartree-Fock-Roothaan momentum distribution in the binary encounter approximation for inner shell ionization

Pramana ◽  
1990 ◽  
Vol 34 (5) ◽  
pp. 447-460
Author(s):  
V Kumar ◽  
S N Chatterjee ◽  
B N Roy
Pramana ◽  
1990 ◽  
Vol 35 (5) ◽  
pp. 485-493 ◽  
Author(s):  
Vijay Kumar ◽  
S K Shrivastava ◽  
B N Roy

1978 ◽  
Vol 56 (9) ◽  
pp. 1255-1260 ◽  
Author(s):  
A. Kumar ◽  
B. N. Roy

Electron impact double ionization cross sections of noble gas atoms have been calculated in the binary encounter approximation by using Gryzinski's double binary encounter model. The correct expression for σΔE including exchange and interference as given by Vriens has been used. Hartree–Fock and hydrogenic velocity distribution functions have been used in considering the ejection of the first and the second atomic electron, respectively. Contribution of ionization from inner-shell has also been taken into account. Calculated values of cross sections are found to be in agreement with the experimental observations.


Author(s):  
Raynald Gauvin ◽  
Gilles L'Espérance

Values of cross sections for ionization of inner-shell electrons by electron impact are required for electron probe microanalysis, Auger-electron spectroscopy and electron energy-loss spectroscopy. In this work, the results of the measurement of inner-shell ionization cross-sections by electron impact, Q, in a TEM are presented for the K shell.The measurement of QNi has been performed at 120 KeV in a TEM by measuring the net X-ray intensity of the Kα line of Ni, INi, which is related to QNi by the relation :(1)where i is the total electron dose, (Ω/4π)is the fractional solid angle, ω is the fluorescence yield, α is the relative intensity factor, ε is the Si (Li) detector efficiency, A is the atomic weight, ρ is the sample density, No is Avogadro's number, t' is the distance traveled by the electrons in the specimen which is equal to τ sec θ neglecting beam broadening where τ is the specimen thickness and θ is the angle between the electron beam and the normal of the thin foil and CNi is the weight fraction of Ni.


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