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Titlebook: Solid-State Physics; An Introduction to P Harald Ibach,Hans Lüth Textbook 19962nd edition Springer-Verlag Berlin Heidelberg 1996 band struc

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Magnetism,ucture were calculated for an electron in an effective potential consisting of the potential of the ion cores and an average potential due to the other electrons. Within this model quite acceptable bandstructures can be calculated. However, another aspect of the one-electron model is more important
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Superconductivity,erials originates from the fact that a real crystal always exhibits deviations from perfect lattice periodicity: phonons and defects. An infinitely high electrical conductivity is unthinkable in this description, because (1) a crystal without a certain degree of disorder is inconceivable according t
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Dielectric Properties of Materials,icroscopic picture one would speak, for instance, of the absorption of a photon via the creation of a phonon or an electron-hole pair. The Maxwellian theory, on the other hand, is a macroscopic approach and the solid is described by material constants. The relation between the two approaches will be
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Textbook 19962nd editionersion in English has already been adopted by many universities in the United States and other countries. This new 2nd edition corresponds to the 4th edition in German. In addition to correcting some typographical errors and making small improvements in the presentation, in the present edition some
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The Electronic Bandstructure of Solids,el is unable to shed any light on the nature of semiconductors and insulators. To make further progress one has to take into account that the electronic states in solids form so-called bands. One can think of these as deriving from the states of the free atom.
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Magnetism,electron model is the basic model for our understanding of the solid state. Furthermore, there are phenomena associated with the collective behavior of the electrons which can nonetheless be tackled within this framework; for example, Thomas-Fermi screening (Sect. 6.5) or the excitation of charge de
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