Introduction to Solid State Physicsproblems after each chapter |
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Page 358
The conductivity of the specimen will be controlled by electrons ( negative charges ) and the material is said to be n type . If acceptors are dominant , holes will be freed in the valence band and the conductivity of the specimen will ...
The conductivity of the specimen will be controlled by electrons ( negative charges ) and the material is said to be n type . If acceptors are dominant , holes will be freed in the valence band and the conductivity of the specimen will ...
Page 422
The essential difference between material for permanent magnets and material for transformer cores lies in the coercive force , which may range from the value of 600 oersteds in a loudspeaker magnet ( Alnico V ) and 20,000 in a special ...
The essential difference between material for permanent magnets and material for transformer cores lies in the coercive force , which may range from the value of 600 oersteds in a loudspeaker magnet ( Alnico V ) and 20,000 in a special ...
Page 471
The material at the boundary between normal and superconducting regions will naturally be in the field Hc , but now the material outside the boundary , such as the material on the surface of the sphere , will see a field less than He ...
The material at the boundary between normal and superconducting regions will naturally be in the field Hc , but now the material outside the boundary , such as the material on the surface of the sphere , will see a field less than He ...
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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