Titlebook: Quantum Electron Theory of Amorphous Conductors; Aleksandr Ivanovich Gubanov Book 1965 Consultants Bureau Enterprises, Inc. 1965 crystal.e

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Band Theory for the Three-Dimensional Model of a Liquid [1],s band structure when the long-range order disappears and there are small departures from the short-range order. In the present chapter, we shall extend this theory to the more realistic case of a three-dimensional model. All the considerations and calculation methods are the same as for the one-dim

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Scattering of Electrons on Thermal Vibrations in a Liquid [1],fically “liquid” scattering, there is, as in crystals, the scattering of electrons on thermal vibrations, which may predominate if the melting point is high. In the present chapter, we shall consider this type of scattering.

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Electrical Conductivity, Thermal Conductivity, Thermoelectric Power, Hall Coefficient, and Nernst Cee path allowing for the scattering due to the departures from long-range order and for the phonon—liquid scattering. However, experimentally we determine not the mean free path, but the electrical conductivity, Hall coefficient, and similar quantities. Since the dependence of the mean free path on

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dermatomyositis

伪造者

Theory of the Electrical Conductivity of Liquid Metals [1, 2],e can also deal with liquid metals by considering them as gases. Although the experimental observations presented in Chap. Ill show that liquids are closer in their structure to crystals than to gases, an approach to the problem of liquid structure is from another viewpoint of great interest.

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