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Titlebook: Introduction to Solid-State Theory; Otfried Madelung Book 1978 Springer-Verlag Berlin Heidelberg 1978 Absorption.band structure.crystal.di

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书目名称Introduction to Solid-State Theory
编辑Otfried Madelung
视频video
丛书名称Springer Series in Solid-State Sciences
图书封面Titlebook: Introduction to Solid-State Theory;  Otfried Madelung Book 1978 Springer-Verlag Berlin Heidelberg 1978 Absorption.band structure.crystal.di
描述.Introduction to Solid-State Theory .is a textbook for graduate students of physics and materials science. It also provides the theoretical background needed by physicists doing research in pure solid-state physics and its applications to electrical engineering. The fundamentals of solid-state theory are based on a description by delocalized and localized states and - within the concept of delocalized states - by elementary excitations. The development of solid-state theory within the last ten years has shown that by a systematic introduction of these concepts, large parts of the theory can be described in a unified way. This form of description gives a "pictorial" formulation of many elementary processes in solids, which facilitates their understanding.   
出版日期Book 1978
关键词Absorption; band structure; crystal; diffusion; dispersion; electron; exciton; kinetics; magnetism; materials
版次1
doihttps://doi.org/10.1007/978-3-642-61885-7
isbn_softcover978-3-540-60443-3
isbn_ebook978-3-642-61885-7Series ISSN 0171-1873 Series E-ISSN 2197-4179
issn_series 0171-1873
copyrightSpringer-Verlag Berlin Heidelberg 1978
The information of publication is updating

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Fundamentals,collective properties of this atomic arrangement. The characteristic properties of free atoms do, of course, determine the nature of the solid they make up, but, when embedded in a crystal lattice, these properties are greatly influenced by the surroundings. Electrical conductivity, ferromagnetism,
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Elementary Excitations,into a sum of one-particle operators. We now want to improve on this approximation by taking . into account. Parts of this interaction were indeed already included in the Hamiltonian (1.32), but we lost important features of it in making the approximations leading to the one-electron model.
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Electron-Phonon Interaction: Transport Phenomena,e . is the band index, . is the wave vector of the electron, and σ is the spin. In this chapter we shall be almost entirely concerned with electrons of one band, the conduction band. Accordingly we need only give the band index explicitly in a few cases. Since for transitions within the conduction b
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