C. Falcony et al., CHARACTERIZATION OF EXCESS SI IN NONSTOICHIOMETRIC SIO2-FILMS BY OPTICAL AND SURFACE-ANALYSIS TECHNIQUES, Journal of the Electrochemical Society, 144(1), 1997, pp. 379-383
Optical and surface analysis techniques such as infrared spectroscopy,
ellipsometry, and Auger electron spectroscopy (AES) and x-ray photoel
ectron spectroscopy (XPS) have been used to study the way in which exc
ess Si is incorporated in nonstoichiometric SiO2 films deposited by a
low pressure chemical vapor deposition technique. It has been found th
at for this range of silicon content, the Si atoms in excess either cl
uster into a well-defined second phase embedded in a SiO2 matrix, or f
orm a SiO2 type of material depending on the postdeposition thermal tr
eatments given to the film. The oxides are deposited at a substrate te
mperature in the range of 650 to 750 degrees C using a mixture of N2O
and SiH4 gases. The excess Si is introduced by reducing the nitrous ox
ide to silane gas ratio during the deposition (this ratio was in the r
ange of 4 to 200). After deposition, a densification process consistin
g of a 1000 degrees C anneal in a nitrogen ambient for 30 min was give
n to some of the samples. The refractive index, as determined by ellip
sometry, is sensitive to the excess of silicon in the films, although
its behavior was similar for both annealed and as-deposited samples. T
he volume percent of excess silicon was estimated using spectroscopic
ellipsometry for some samples. Infrared spectroscopy, on the other han
d, shows a clear shift of the stretching vibration peak of Si-O-Si bon
ds toward lower wave numbers as the Si excess in the film is increased
in the case of as-deposited films, while the annealed samples do not
present this effect. Also, as-deposited samples show an absorption pea
k, at 890 cm(-1), that could be associated with partially oxidized sil
icon. AES and XPS spectra show a distinct difference in the peaks asso
ciated to Si bonded to either oxygen or another silicon atom for both
types of samples indicating that at least a considerable part of the e
xcess Si in the as-deposited samples is in the form of SiOx, while in
the annealed samples it is mostly forming a second phase within a sili
con dioxide matrix.