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 be
controlled ...
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 be
controlled ...
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
high ...
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
high ...
Page 471
48 ) H > H . When this situation occurs we can avoid having the whole sphere
become normal by having the material around the equator of the sphere become
normal ; the effective shape of the superconducting material will then become ...
48 ) H > H . When this situation occurs we can avoid having the whole sphere
become normal by having the material around the equator of the sphere become
normal ; the effective shape of the superconducting material will then become ...
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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 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