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

方言

書目名稱Electrons in Metals and Semiconductors影響因子(影響力)




書目名稱Electrons in Metals and Semiconductors影響因子(影響力)學(xué)科排名




書目名稱Electrons in Metals and Semiconductors網(wǎng)絡(luò)公開度




書目名稱Electrons in Metals and Semiconductors網(wǎng)絡(luò)公開度學(xué)科排名




書目名稱Electrons in Metals and Semiconductors被引頻次




書目名稱Electrons in Metals and Semiconductors被引頻次學(xué)科排名




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書目名稱Electrons in Metals and Semiconductors年度引用學(xué)科排名




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書目名稱Electrons in Metals and Semiconductors讀者反饋學(xué)科排名

d-limonene

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 ..

ANT

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.

BADGE

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.

MIRTH

Amendment

Amendment

,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.

Meager

小溪

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

很是迷惑

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.