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 capacity ; such
...
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 capacity ; such
...
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 530
When irradiated with light near 2490 A , a transition A + B to the upper state may
take place . According to the Franck - Condon principle the transition occurs with
the lattice configuration characteristic of the ground state : thus the absorption ...
When irradiated with light near 2490 A , a transition A + B to the upper state may
take place . According to the Franck - Condon principle the transition occurs with
the lattice configuration characteristic of the ground state : thus the absorption ...
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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 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