Titlebook: Basic Semiconductor Physics; Chihiro Hamaguchi Textbook 20011st edition Springer-Verlag Berlin Heidelberg 2001 Energy band structures.Lumi

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Optical Properties 1,ic field intensity vector ., magnetic field flux (referred to as “magnetic field” in this text) ., current density ., and charge density .; then the macroscopic domain is governed by the classical field equations of Maxwell: ., ., ., ..

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,Electron—Phonon Interaction and Electron Transport,tions at finite temperatures because of their thermal motion. When a atom is displaced from its equilibrium position, the atom is subject to a restorating force depending on the displacement. The restorating force follows Hooke’s law and is proportional to the displacement. When each atom vibrates r

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Magnetotransport Phenomena,cular to both the current and the magnetic field. This phenomena was discovered in 1879 by E.H. Hall and is called the .. This phenomena has been successfully used to investigate the electronic properties of semiconductors and metals. In this section, first we deal with the Hall effect in a simple w

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Quantum Structures, initiated in the 1960s, when electrons in the inversion layer of the MOSFET (Metal-Oxide-Semiconductor Field Effect Transistor) were found to be quantized at the interface and to exhibit two-dimensional properties. Then the Quantum Hall effect was discovered in 1980 by van Klitzing et al. [8.15] by

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Springer Series in Solid-State Sciencesplayed a very important role in understanding the valence band structures of Ge and Si and later led to an accurate determination of the energy band structures. In this chapter first we will describe the cyclotron resonance experiment and its analysis in order to discuss the anisotropy of the electr

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