The coefficient of electron backscattering, the angular and energy dis
tribution of transmitted electrons and of backscattered electrons have
been calculated by the Monte-Carlo method using several models of ele
ctron elastic scattering. The calculations were carried out for C, Al,
Cu, Au, in the 10-100 keV energy range and in the 20-1000 nm film thi
ckness range. Our findings were compared with published experimental r
esults. The cross-section of elastic scattering was calculated either
by Rutherford's formula (the screened atomic potential was assumed) or
by Mott's theory including electron spin, or was taken from data tabl
es computed from Hartree-Fock atomic wave functions. This provided an
opportunity to decide which model of electron-atom elastic interaction
is the best for simulation. The results showed that the backscatterin
g coefficient, and mainly its dependence on him thickness and electron
energy, is a quantity which is strongly sensitive to the model type.
The best agreement between calculated and experimental data was reache
d, in the full range of primary electron energies and film thicknesses
, for Au and Al by using tables with rigorous partial wave calculation
s and for Cu by using Rutherford's formula, even though the difference
s among results for Cu are relatively small.