Introduction to Solid State Physicsproblems after each chapter |
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Page 35
SIMPLE CRYSTAL STRUCTURES We discuss briefly a small number of simple crystal structures of general interest , including the hexagonal close - packed , diamond , cubic zinc sulfide , sodium chloride , cesium chloride , and fluorite ...
SIMPLE CRYSTAL STRUCTURES We discuss briefly a small number of simple crystal structures of general interest , including the hexagonal close - packed , diamond , cubic zinc sulfide , sodium chloride , cesium chloride , and fluorite ...
Page 132
If the mass ratio m / M is » 1 , however , the total spread in frequency of the optical branch becomes quite small ; this fact suggests a simple approximation to the heat capacity . If the total number of atoms is 2N , we treat the N ...
If the mass ratio m / M is » 1 , however , the total spread in frequency of the optical branch becomes quite small ; this fact suggests a simple approximation to the heat capacity . If the total number of atoms is 2N , we treat the N ...
Page 422
The termination structures revealed by powder patterns are often more complicated than the simple cases we have discussed , but domain structure always has its origin in the possibility of lowering the energy of a system by going from a ...
The termination structures revealed by powder patterns are often more complicated than the simple cases we have discussed , but domain structure always has its origin in the possibility of lowering the energy of a system by going from a ...
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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