Introduction to Solid State Physicsproblems after each chapter |
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Page 247
The allowed energy levels are quantized in this way , other values of the energy being excluded as the corresponding y's do not satisfy the boundary conditions . It is often convenient , particularly in three dimensions , to introduce ...
The allowed energy levels are quantized in this way , other values of the energy being excluded as the corresponding y's do not satisfy the boundary conditions . It is often convenient , particularly in three dimensions , to introduce ...
Page 286
To satisfy these two conditions the normal derivative au / an must vanish on the boundary planes of each polyhedron . ... The cubes show the unit cells in either case . sphere is determined by the condition that the volume of the s ...
To satisfy these two conditions the normal derivative au / an must vanish on the boundary planes of each polyhedron . ... The cubes show the unit cells in either case . sphere is determined by the condition that the volume of the s ...
Page 373
It is interesting to state in terms of the mobility the condition wt > 1 for the observation of cyclotron resonance . In esu , T = m * u / e ; to have wr > 1 requires u > e / wm * . For For f = 24,000 mc / sec , the condition on ...
It is interesting to state in terms of the mobility the condition wt > 1 for the observation of cyclotron resonance . In esu , T = m * u / e ; to have wr > 1 requires u > e / wm * . For For f = 24,000 mc / sec , the condition on ...
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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