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Titlebook: Electronic Properties of Materials; Rolf E. Hummel Book 1993Latest edition Springer-Verlag Berlin Heidelberg 1993 ceramics.crystal.electro

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发表于 2025-3-21 19:14:19 | 显示全部楼层 |阅读模式
书目名称Electronic Properties of Materials
编辑Rolf E. Hummel
视频video
图书封面Titlebook: Electronic Properties of Materials;  Rolf E. Hummel Book 1993Latest edition Springer-Verlag Berlin Heidelberg 1993 ceramics.crystal.electro
描述It is quite satisfying for an author to learn that his brainchild has been favorably accepted by students as well as by professors and thus seems to serve some useful purpose. This horizontally integrated text on the electronic properties of metals, alloys, semiconductors, insulators, ceramics, and poly­ meric materials has been adopted by many universities in the United States as well as abroad, probably because of the relative ease with which the material can be understood. The book has now gone through several re­ printing cycles (among them a few pirate prints in Asian countries). I am grateful to all readers for their acceptance and for the many encouraging comments which have been received. I have thought very carefully about possible changes for the second edition. There is, of course, always room for improvement. Thus, some rewording, deletions, and additions have been made here and there. I withstood, how­ ever, the temptation to expand considerably the book by adding completely new subjects. Nevertheless, a few pages on recent developments needed to be inserted. Among them are, naturally, the discussion of ceramic (high-tempera­ ture) superconductors, and certain elements
出版日期Book 1993Latest edition
关键词ceramics; crystal; electron; electronics; electrons; energy; magnetic properties; magnetism; optoelectronics
版次2
doihttps://doi.org/10.1007/978-94-017-4914-5
isbn_softcover978-81-7319-021-6
isbn_ebook978-94-017-4914-5
copyrightSpringer-Verlag Berlin Heidelberg 1993
The information of publication is updating

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The Schrödinger Equationof an electron as a wave, as suggested by Schrödinger in 1926. All “derivations” of the Schrödinger equation start in one way or another from certain assumptions which cause the uninitiated reader to ask the legitimate question, “Why just in this way?” The answer to this question can naturally be gi
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Electrons in a Crystal cases an outer, i.e., a valence, electron. However, in a solid of one cubic centimeter at least 10. electrons can be found. In this section we shall describe how these electrons are distributed among the available energy levels. It is impossible to calculate the exact place and the kinetic energy o
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Electrical Conduction in Polymers, Ceramics, and Amorphous Materialsics industry, e.g., as handles for a variety of tools, as coatings of wires, or for casings of electrical equipment. Most polymeric materials have the required insulating properties and have been used for decades for this purpose. It came, therefore, as a surprise when it was discovered that some po
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Atomistic Theory of the Optical Propertiese continuum theory considers only macroscopic quantities and interrelates experimental data. No assumptions are made about the structure of matter when formulating equations. Thus, the conclusions which have been drawn from the empirical laws in Chapter 10 should have general validity as long as not
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Quantum Mechanical Treatment of the Optical Propertiesh equations which reproduce the optical spectra of solids reasonably well. Unfortunately, the treatment had one flaw: For calculation and interpretation of the infrared (IR) absorption we used the concept that electrons in metals are free; whereas the absorption bands in the visible and ultraviolet
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Applicationsicularly metals) are opaque so that the measurements have to be taken in reflection. Light penetrates about 10 nm into a metal (see Table 10.1). As a consequence, the optical properties are basically measured near the surface which is susceptible to oxidation, deformation (polishing), or contaminati
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