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Electronic structure of wurtzite cadmium sulfideStoffel, Ned G. January 1983 (has links)
Thesis (Ph. D.)--University of Wisconsin--Madison, 1983. / Typescript. Vita. Description based on print version record. Includes bibliographical references (leaves 127-133).
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Cathodic depositions of the compound semiconductor cadmium sulfideRichard, Jeffrey B. 01 January 1985 (has links)
Thin layer deposits of cadmium sulfide (CdS) for photovoltaic purposes can be made by cathodic deposition from a nonaqueous solution. There were numerous parameters that were controlled in this electro-deposition. Several of these parameters, including temperature, current density, reactant concentrations and impurity level doping, were studied and optimized. The mechanism of this deposition process is not fully understood, mainly due to the complex chemistry of sulfur. Part of this complexity is the presence of S(,6) and S(,7) along with the major component of S(,8) in sulfur solutions. At 90(DEGREES), these minor species constitute 2% of the total sulfur. Electrochemical studies were made on these species with gold, porous carbon and CdS single crystal electrodes. These showed that S(,6) and S(,7) are electrochemically more reactive than S(,8). Furthermore, they may be the main reacting species in CdS formation, even though they are present at such low levels. Adsorption of all species of sulfur was noted at room temperature and this adsorption may be causing excess sulfur to be incorporated into the CdS deposits. There has been an important development in the measurement of impurity levels of semiconductors called electrochemical photocapacitance spectroscopy. It can be used to analyze impurity levels in a wide variety of semiconductors by shining subband gap light on the semiconductor in a photoelectrochemical cell while measuring the capacitance on the surface. Interpretation of these spectra has previously been qualitative. A quantitative model was developed here along with a computer program utilizing this interpretation. Several types of semiconductors were analyzed by this technique, including these CdS deposits which showed impurity levels that may be due to excess sulfur. Other types of compound semiconductors can also be made by this cathodic deposition. It is hoped that the information gathered here can be used to improve these other semiconductor depositions as well as CdS.
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Measurement and interpretation of potential distributions in photoconductive CdSMiller, Robert Frank, January 1957 (has links)
Thesis (Ph. D.)--University of Wisconsin--Madison, 1957. / Typescript. Abstracted in Dissertation abstracts, v. 17 (1957) no. 8, p. 1792. Vita. eContent provider-neutral record in process. Description based on print version record. Includes bibliographical references (leaves 74-75).
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Measurement and interpretation of transient electronic phenomena in cadmium sulfideGreiner, Richard Anton, January 1957 (has links)
Thesis (Ph. D.)--University of Wisconsin--Madison, 1957. / Typescript. Vita. eContent provider-neutral record in process. Description based on print version record. Includes bibliographical references (leaves 89-93).
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Series assignments in the fluorescence line spectra of high purity cadmium sulfide /Greene, Lawrence Conde January 1967 (has links)
No description available.
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Cyclotron resonance in cadmium sulfideBaer, Walter S., January 1964 (has links)
Thesis (Ph. D.)--University of Wisconsin, 1964. / Typescript. Vita. eContent provider-neutral record in process. Description based on print version record. Bibliography: leaves 87-91.
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Temperature dependence of ESR in CdS (I)Perkin, Ronald Gordon January 1970 (has links)
Previous measurements on CdS (I) have shown a temperature shift in the single electron spin resonance (ESR) impurity band line. At 34 GHz this shift was found to be:
dg= - 2.5 x 10ˉ ⁴/°K
dT
in going from 4.2°K to 1.7°K.
This thesis presents the construction and testing of a metal temperature controlled dewar for the purpose of measuring the shift over the temperature range from 40°K to 1.7°K using an X-band (9 GHz)spectrometer. The signal was observed between 1.7°K and 4.2°K but rapidly broadened and could not be seen at higher temperatures. Since the lowest attainable temperature of the metal dewar was around 5°K, it could not be used as planned. Further studies using glass dewars proved that the g-shift at 9 GHz was too small, to be measured.
The theory for the g-shift is discussed and the performance of the dewar evaluated. / Science, Faculty of / Physics and Astronomy, Department of / Graduate
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ESR study of antimony doped cadmium sulphideHalliwell, Robin Ernest January 1969 (has links)
The electronic g-tensor in antimony doped cadmium sulphide has been measured at 1.1°K. A sample doped to a room temperature resistivity of 3.3 ohm-cm exhibited an anisotropic g-tensor with g// = 1.788 and g⊥ = 1.770.
A single asymmetric line was observed. The asymmetry of this line was found to decrease with decreasing incident power. Further experiments to study this line shape are indicated. / Science, Faculty of / Physics and Astronomy, Department of / Graduate
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Diffusion and luminescence of rare earths in cadmium sulfide /Girton, Dexter George January 1969 (has links)
No description available.
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Surface potentials of sensitization systems and the mechanisms of spectral sensitization /Freeman, Garth Bowen January 1974 (has links)
No description available.
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