Introduction to Solid State Physicsproblems after each chapter |
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Page 199
Schematic variation of spontaneous polarization and reciprocal susceptibility for
first order ( case B ) and second order ( case A ) transitions . The transition in
barium titanate is first order , but is close to being second order . thermodynamic
...
Schematic variation of spontaneous polarization and reciprocal susceptibility for
first order ( case B ) and second order ( case A ) transitions . The transition in
barium titanate is first order , but is close to being second order . thermodynamic
...
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
bands will be ...
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
bands will be ...
Page 459
Charles Kittel. Occurrence of superconductivity . 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 ...
Charles Kittel. Occurrence of superconductivity . 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 ...
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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