Diffraction and other structural measurements on n-type SiC thin films prepared in a TCDDC (two consecutive decomposition and deposition chamber) system indicate the presence of Si microcrystals (without evidence for SiC crystallites). Weakly absorbing, highly conductive layers (σ ≥ 10-1 (Ω-cm)-1) contain up to 20 at.% C and 25 at.% O. The optoelectronic properties of these films can be explained in terms of a sufficient volume fraction (above the percolation threshold) of Si microcrystals surrounded by an a-Si:C:O:H matrix.

The influence of U.V. light on the transport properties of a-Si : H films during its growth in a r.f. double chamber system was investigated by conductivity, optical absorption, I.R. absorption, spectral photoconductivity and X-ray diffraction measurements. It was concluded that the presence of U.V. light during the deposition process controls the way how hydrogen is incorporated in the structure as well as the impurity atoms. The microcrystalline films investigated present sharp peaks in the I.R. spectra. Both boron and phosphorus doped films show conductivities higher than 10 S cm-1 and estimated crystalline sizes of the order of 80 Å. © 1987.

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Doped and undoped a-Si:H and a-SiC:H films were deposited by R. F. decomposition of silane and silane/methane mixtures respectively, in a two consecutive (decomposition and deposition) chambers glow discharge capacitively coupled system. Their electro-optical properties were extensively investigated through dark conductivity, photoconductivity, spectral response, optical absorption, R. F. transmission spectra, electron spin ressonance and CxV MOS measurements.

A double-chamber system was used to deposit large-area hydrogenated amorphous silicon films for photovoltaic applications. The electro-optical characterisation of films of area 400 cm2 deposited on glass substrates is described in this paper. The deposition rate of the films is dependent on the r.f. power delivered, the substrate bias and the partial pressure of the reactive gas. The film thickness was observed to have a uniformity of better than 0.5%. The best film quality was obtained for a deposition rate of about 1.5 Å s-1. The optical gap, activation energy, photosensitivity, density of gap states and hydrogen content were determined. © 1985.