Introduction to Solid State Physicsproblems after each chapter |
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Page 202
Frequency dependence of the real part of the dielectric constant in barium titanate , from smoothed data of von Hippel and Powles and Jackson . spaced only 10-2 cm apart . This feature is of great importance in the application of ...
Frequency dependence of the real part of the dielectric constant in barium titanate , from smoothed data of von Hippel and Powles and Jackson . spaced only 10-2 cm apart . This feature is of great importance in the application of ...
Page 304
The values of the conductivity for T » calculated in this way from ( 11.89 ) are of the correct order of magnitude for monovalent metals and have the correct temperature dependence . The extension of the theory to the region T « is ...
The values of the conductivity for T » calculated in this way from ( 11.89 ) are of the correct order of magnitude for monovalent metals and have the correct temperature dependence . The extension of the theory to the region T « is ...
Page 327
7 VARIATION OF HALL CONSTANT The dependence of the Hall coefficient on alloy composition should Hall coefficient x 104 0.40 bcc O 10 0.30 20 30 % Sn fcc -1 N ( E ) Electrons per atom per ev 0.20 -2 - 3 0.10 - 4 1 2 3 4 5 6 7 8 9 -5 ...
7 VARIATION OF HALL CONSTANT The dependence of the Hall coefficient on alloy composition should Hall coefficient x 104 0.40 bcc O 10 0.30 20 30 % Sn fcc -1 N ( E ) Electrons per atom per ev 0.20 -2 - 3 0.10 - 4 1 2 3 4 5 6 7 8 9 -5 ...
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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