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The temperature oscillation method was used to synthesize dense single-phase polycrystalline AgGaS2 from high purity elements. AgGaS2 single crystal of 8 mm diameter and 45 mm length, free of voids and crack was obtained by the descending ampoule with steady ampoule rotation method using the synthesized polycrystalline charge. The grown crystal was subjected to powder X-ray diffraction and single crystal X-ray diffraction. The AgGaS2 has been studied using differential scanning calorimetry (DSC) technique. The single crystal has high transmission of 75% in the Mid IR region. The band gap energy was calculated using absorption spectrum. The stoichiometric composition of AgGaS2 was measured using energy dispersive spectrometry (EDAX). The structural and compositional uniformities of AgGaS2 were studied using micro-Raman scattering spectroscopy at room temperature. The photoluminescence behavior of AgGaS2 has been analyzed. It shows the maximum emission at 538 nm. The resistivity of the grown single crystal has been measured. 相似文献
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Single crystal of the ternary semi-conductor AgInSe2 has been grown by Bridgman technique. The AgInSe2 crystal crystallizes in the tetragonal chalcopyrite structure. Using melt temperature oscillation method polycrystalline charge was synthesized. The synthesized charge was subjected to powder X-ray diffraction analysis. Thermal property of AgInSe2 was analyzed using differential scanning calorimetry (DSC) technique. The melting and solidification temperature is 777 °C and 761 °C respectively. The synthesized polycrystalline charge was employed to grow AgInSe2 single crystals. The grown crystal was confirmed by single crystal X-ray diffraction. The crystal exhibits 60% transmission in the Infrared region. The stoichiometric composition of AgInSe2 was confirmed by Energy dispersive X-ray analysis (EDAX). The electrical properties of the crystal were studied by Hall Effect measurements and photoconductivity. 相似文献
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We have prepared HxWOy amorphous thin films both by evaporation of tungsten trioxide powder and by cathodic sputtering of a tungsten target in an
argon/oxygen/hydrogen reactive gas mixture. The evaporated layers have the composition HxWO2.7 (0.2 < × < 0.5). Their oxygen content seems rather insensitive to the evaporation parameters. We do not observe any correlation
between x and these parameters. Evaporated virgin layers are nearly transparent. Annealing,under vacuum leaves y unchanged,
under oxygen increases y to 3. Annealing of the virgin layer under vacuum induces the growth of the 1.38 eV absorption band
(giving blue coloration) and a decrease of the activation energy for conduction. Annealing the blue layers in oxygen destroys
the 1.38 eV band and increases the activation energy for conduction. In both cases annealing at high temperature induces a
microcrystalline phase with an absorption band centered about 0.72 eV (giving also a blue coloration) and a jump in electronic
conductivity. As in the case of the 1.38 eV band, an increase of the intensity of the 0.72 eV band induces a decrease of the
activation energy for conduction. The two bands are interpreted as polaronic like. They can be induced in transparent layers
without any change in global composition by excitation of the hydrogen atoms from a “ passive” state to an “ active” state.
In addition to the hydrogen content, the existence of the 1.38 eV band requires some substoichiometry. The study of the optical
and electrical properties of amorphous HxWOy sputtered layers, supports our previous conclusions about the composition range (C) for the coloration capability of transparent
thin films. In addition there is a composition range (B) where the virgin layers are blue, and a composition range (M) where
they have a metallic like behavior. On the other side of (C), there is a range (C’) where uv illumination only induces a decrease
in the activation energy for conduction, then a range (T) where the layers are completely nonresponsive. One can pass from
(T) to (B) through (C') and (C) either at constant hydrogen content by increasing the departure from stochiometry, or at constant
substoichiometry by increasing the hydrogen content.
A part of this work was presented at EMC Cornell, New York July 1, 1977. 相似文献
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C. L. Littler B. P. Gorman D. F. Weirauch P. K. Liao H. F. Schaake 《Journal of Electronic Materials》2005,34(6):768-772
Transmission spectra of liquid-phase epitaxy (LPE) Hg1-xCdxTe with Cd mole fractions in the range of 0.23<x<0.30 have been obtained as a function of temperature and thickness. The results
are described using a model consisting of exponential (Urbach) absorption in the band tail region and band-to-band absorption,
predicted by a Kane k p model, for the above band gap region. Modifications to the Urbach and transmission expressions are
found to be necessary to properly describe the shape, temperature, and thickness dependence of the spectra. A known composition
gradient was found to be sufficient to describe the spectra obtained for thin (<20-μm) samples. 相似文献