Introduction to Solid State Physicsproblems after each chapter |
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Page 58
ROTATING - CRYSTAL METHOD A simple rotating - crystal camera is shown in
Fig . 2.12 . The film is mounted with cylindrical geometry concentric with a rotating
spindle on which the single crystal specimen is mounted . The dimensions of ...
ROTATING - CRYSTAL METHOD A simple rotating - crystal camera is shown in
Fig . 2.12 . The film is mounted with cylindrical geometry concentric with a rotating
spindle on which the single crystal specimen is mounted . The dimensions of ...
Page 182
8 Ferroelectric Crystals A ferroelectric crystal is defined as a crystal which
exhibits a spontaneous electric dipole moment ; in other words , a crystal for
which even in the absence of an applied electric field the center of positive
charge does not ...
8 Ferroelectric Crystals A ferroelectric crystal is defined as a crystal which
exhibits a spontaneous electric dipole moment ; in other words , a crystal for
which even in the absence of an applied electric field the center of positive
charge does not ...
Page 522
In this estimate we are taking the dielectric constant of the crystal as unity . Thus n
= 1 / 4we = 2 X 108 electrons cm ? This figure is comparable with the amount of
charge piled up by a current density of 10 ua / cm2 flowing for 3 usec , as the ...
In this estimate we are taking the dielectric constant of the crystal as unity . Thus n
= 1 / 4we = 2 X 108 electrons cm ? This figure is comparable with the amount of
charge piled up by a current density of 10 ua / cm2 flowing for 3 usec , as the ...
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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