Introduction to Solid State Physicsproblems after each chapter |
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Page 199
The transition in barium titanate is first order , but is close to being second order . thermodynamic methods that a case A transition does not have a latent heat of transition , but is rather accompanied by a discontinuity in the heat ...
The transition in barium titanate is first order , but is close to being second order . thermodynamic methods that a case A transition does not have a latent heat of transition , but is rather accompanied by a discontinuity in the heat ...
Page 295
The metals of the transition groups of the periodic table are known to have unfilled inner shells , and the corresponding bands may be unfilled . As the overlap of inner shells on adjacent atoms is likely to be relatively small ...
The metals of the transition groups of the periodic table are known to have unfilled inner shells , and the corresponding bands may be unfilled . As the overlap of inner shells on adjacent atoms is likely to be relatively small ...
Page 459
The superconducting elements and their transition temperatures are listed in Table 16.1 . The features to be noted are : ( a ) Monovalent metals are not superconductors . ( b ) The ferromagnetic and antiferromagnetic metals are not ...
The superconducting elements and their transition temperatures are listed in Table 16.1 . The features to be noted are : ( a ) Monovalent metals are not superconductors . ( b ) The ferromagnetic and antiferromagnetic metals are not ...
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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