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Titlebook: Electrons in Metals and Semiconductors; R. G. Chambers Book 1990 R.G. Chambers 1990 Potential.atoms.density.dynamics.electron.electrons.he

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发表于 2025-3-21 17:59:21 | 显示全部楼层 |阅读模式
书目名称Electrons in Metals and Semiconductors
编辑R. G. Chambers
视频video
丛书名称Physics and Its Applications
图书封面Titlebook: Electrons in Metals and Semiconductors;  R. G. Chambers Book 1990 R.G. Chambers 1990 Potential.atoms.density.dynamics.electron.electrons.he
描述Solid-state physics has for many years been one of the largest and most active areas of research in physics, and the physics of metals and semiconductors has in turn been one of the largest and most active areas in solid-state physics. Despite this, it is an area in which new and quite unexpected phenomena - such as the quantum Hall effect - are still being discovered, and in which many things are not yet fully understood. It forms an essential part of any undergraduate physics course. A number of textbooks on solid-state physics have appeared over the years and, because the subject has now grown so large, the books too have usually been large. By aiming at a more limited range of topics, I have tried in this book to cover them within a reasonably small compass. But I have also tried to avoid the phrase ‘It can be shown that. . . ‘, as far as possible, and instead to explain to the reader just why things are the way they are; and sometimes this takes a little longer. I hope that some readers at least will find this approach helpful. 1 The free-electron model 1. 1 THE CLASSICAL DRUDE THEORY The characteristic properties of metals and semiconductors are due to their conduction electr
出版日期Book 1990
关键词Potential; atoms; density; dynamics; electron; electrons; heat; metals; model; physics; semiconductor
版次1
doihttps://doi.org/10.1007/978-94-009-0423-1
isbn_softcover978-0-412-36840-0
isbn_ebook978-94-009-0423-1
copyrightR.G. Chambers 1990
The information of publication is updating

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发表于 2025-3-21 22:55:36 | 显示全部楼层
Jun Liu,Jian-Bo Yang,Jin Wang,How-Sing Sii signal. But in determining the transport properties of metals and semiconductors — for example their electrical and thermal conductivities σ and . — collisions are all-important; if there were no collisions, the relaxation time τ would be infinite, and so therefore would σ and ..
发表于 2025-3-22 01:59:51 | 显示全部楼层
Intelligent Systems for Engineeringnd the empty conduction bands above ε. (Fig. 5.9). Because of this gap, the number of carriers (electrons and holes) varies rapidly with temperature in a semiconductor, whereas it is essentially temperature-independent in a metal, and our first task is to look at this temperature variation.
发表于 2025-3-22 05:48:05 | 显示全部楼层
Crystal Structures and the Reciprocal Lattice,y tiny crystals form, and these then grow together to form a solid polycrystalline mass. By cooling slowly and carefully, one can instead grow large single crystals, and single crystals of silicon, for example, have long been the starting material for the semiconductor industry.
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发表于 2025-3-22 17:41:05 | 显示全部楼层
,Management — A Distributed Function,In this chapter, we shall look at the thermal and electrical properties of the Sommerfeld free-electron model, starting with the electronic heat capacity.
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发表于 2025-3-23 03:18:08 | 显示全部楼层
https://doi.org/10.1007/978-981-19-8253-8In Chapter 2 we were concerned only with free electrons, for which . = ., and we assumed that the effect of fields . and . on an electron moving with velocity . was given by the Lorentz force equation
发表于 2025-3-23 08:13:06 | 显示全部楼层
https://doi.org/10.1007/978-3-642-80484-7Now that we have looked at the effect of electric fields and of collisions separately, we can look at the effect of the two together, and see how they determine the conductivity and other transport properties. We consider metals in this and the following three chapters, and then turn to semiconductors.
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