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A description of the classical Drude-Zener theory of the dielectric constant and conductivity of a conductor is given, with particular reference to germanium and other semiconductors. The degree of agreement between theory and experiment is indicated. Methods whereby the conductivity of a semiconductor may be modulated and the application of these techniques to the study of the optical and microwave properties of semiconductors are described.
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A F Gibson (1958) studied this question.
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