Application of Solar Energy 132 -C, was controlled using a thermocouple with an accuracy of ± C. The optimum distance from the atomizer to the substrate and the compressed air pressure were cm and . kg/cm , respectively. Figure shows schematically the equipment set-up.
. Characterization equipment and methodsThe film thickness was measured with an "lpha Step electronic profilometer. The electrical resistivity, Hall mobility and carrier concentration were measured at room temperature using the van der Pauw method. Hall effect parameters were recorded for a magnetic field of . Tesla. The optical transmission spectrum was obtained using a spectrophotometer. The structural characterization was carried out with an X-ray diffractometer operating in the "ragg-"rentano Θ-Θ geometry with Cu K α radiation. " JSPM atomic force microscope was used to study the film surfaces. The chemical composition of the films was determined using an UHV system of VG Microtech ESC" Multilab, with an "l-K α X-ray source . eV and a CL"M MCD analyzer.
. Properties of the spray deposited ITO filmsThe X-ray diffraction XRD measurements shown in Figure indicate that all deposited ITO films, with thicknesses in the -nm range, and fabricated from the chemical solutions for different Sn/In ratios, presents a cubic bixebyte structure in a polycrystalline configuration with as the preferential grain orientation 2 (grad) Figure 6. XRD spectra of the ITO films fabricated using precursors with different Sn/In ratios. The mean size of the grains, 30-50 nm, was determined using the classical Debye-Scherrer formula from the half-wave of the (400) reflections of the XRD patterns." surface roughness of about nm was determined from images of the film surfaces obtained with an atomic force microscope Figure . The use of sapphire substrates allows for determining the optical energy gap of the ITO films by the extrapolation of the linear part of the α ν curves to α = , where α is the absorption coefficient. The optical gap increases with the carrier concentration due to the well known Moss-"urstein shift. For ITO films fabricated using the solution with a % Sn/In ratio, this shift is . eV, and the optical gap is . ± . eV. Such high value of the optical gap offers transparency in the ultraviolet range, which is of fundamental importance in solar cell applications. "ecause of the opposite dependence of conductivity and transmission T of the ITO film on its thickness t , both parameters must be optimized. " performance comparison of different films is possible using ϕ TC = T / R ψ = texp − at as a figure of merit [ ]. Metal to form an ohmic contact in the back side of the wafer was deposited on the n + -layer previously created by diffusion. The device area for measurements was -cm . "pproximately, a μm Cr/Cu/Cr film was evaporated through a metal mask to make a grid pattern of approximately grid lines/cm. "fter the fabrication, the capacitance-voltage characterization was conducted in order to control the value of the potential barrier. Then the following...