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
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 ...
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 390
crystal is pulled slowly from a melt of molten germanium as the crystal is being
grown . If the melt initially has an excess of donor impurities the crystal will be n
type . At a certain stage of the process acceptor impurities are suddenly added to
...
crystal is pulled slowly from a melt of molten germanium as the crystal is being
grown . If the melt initially has an excess of donor impurities the crystal will be n
type . At a certain stage of the process acceptor impurities are suddenly added to
...
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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