Jw. Park et al., IRRADIATION-INDUCED DECOMPOSITION OF AL2O3 DURING AUGER-ELECTRON SPECTROSCOPY ANALYSIS, Journal of vacuum science & technology. A. Vacuum, surfaces, and films, 14(2), 1996, pp. 286-292
Citations number
16
Categorie Soggetti
Physics, Applied","Materials Science, Coatings & Films
The effect of electron fluence on the decomposition of sapphire (Al2O3
) was studied in situ by Auger electron spectroscopy (AES). The decomp
osition was primarily detected by monitoring the evolution of the low
kinetic energy Auger transitions of aluminum in Al2O3 (54 eV) and in m
etallic aluminum (68 eV). The decomposition of sputter-cleaned sapphir
e started at a fluence of similar to 4.9 x 10(19) electrons/cm(2) (7.8
C/cm(2)). This fluence was independent of the electron fluxes used in
this work, except the lowest, which indicates that heating due to ele
ctron bombardment does not significantly affect the decomposition beha
vior. Electron-induced decomposition takes place in a minimum of the f
irst five atomic layers of the substrate, as revealed by the evolution
during irradiation of the high energy Al peaks associated with Al2O3
(1388 eV) and metallic aluminum (1396 eV). Comparison of the evolution
of low and high kinetic energy Auger transitions demonstrates that th
e decomposition kinetics are much faster for the first monolayer than
for the subjacent atomic layers. The surface condition strongly influe
nces the decomposition kinetics. Thus, a carbon layer adsorbed at the
alumina surface significantly increases the threshold dose for decompo
sition. The carbon layer most probably acts as a diffusion barrier for
the oxygen produced during decomposition. An equation for the decompo
sition rate of the first monolayer of alumina is established. The inte
gral of this equation gives a good fitting to the experimental data. I
t is found that the Auger signal of aluminum from sapphire does not di
sappear even if the entire region has been decomposed. This effect is
due to backscattered electrons that promote Auger electron excitations
outside the irradiated region. (C) 1996 American Vacuum Society.