Introduction to Solid State Physicsproblems after each chapter |
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Page 164
M ELECTRONIC POLARIZABILITIES The total polarizability of an atom or ion may usually be separated into three parts : 5 electronic , ionic , and orientational . The electronic contribution arises from the displacement of electrons in an ...
M ELECTRONIC POLARIZABILITIES The total polarizability of an atom or ion may usually be separated into three parts : 5 electronic , ionic , and orientational . The electronic contribution arises from the displacement of electrons in an ...
Page 360
However , we cannot usually determine the donor ionization energy by measuring the conductivity or , better , the Hall coefficient in the limit in which ( 13.40 ) applies . At low temperatures there are usually fewer conduction ...
However , we cannot usually determine the donor ionization energy by measuring the conductivity or , better , the Hall coefficient in the limit in which ( 13.40 ) applies . At low temperatures there are usually fewer conduction ...
Page 384
The seed is usually rotated at about 100 rpm . The final crystal may weigh several pounds . For further details of the manufacture of transistor materials the reader is referred to Chapter 13 of the book by Coblenz and Owens listed at ...
The seed is usually rotated at about 100 rpm . The final crystal may weigh several pounds . For further details of the manufacture of transistor materials the reader is referred to Chapter 13 of the book by Coblenz and Owens listed at ...
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Contents
DIFFRACTION OF XRAYS BY CRYSTALS | 44 |
CLASSIFICATION OF SOLIDS LATTICE ENERGY | 63 |
ELASTIC CONSTANTS OF CRYSTALS | 85 |
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alloys applied approximately associated atoms axis band boundary calculated cell chapter charge concentration condition conductivity consider constant crystal cubic density dependence determined dielectric diffusion direction discussion dislocation distribution domain effect elastic electric electron elements energy equal equation equilibrium experimental expression factor field force frequency function germanium give given heat capacity hexagonal holes important impurity increase interaction ionic ions lattice levels London magnetic magnetic field mass material measurements metals method motion normal observed obtained parallel particles Phys physics plane polarization positive possible potential present problem properties range reference reflection region relation resistivity result room temperature rotation shown in Fig simple solid solution space space group specimen structure surface symmetry Table temperature theory thermal tion transition unit usually values vector volume wave zero zone