Introduction to Solid State Physicsproblems after each chapter |
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Page 157
The interaction of the local field with the atom determines the polarization , yet the local field may itself be a function of the polarization . We then discuss the electric polarization of atoms , molecules , and crystals in static ...
The interaction of the local field with the atom determines the polarization , yet the local field may itself be a function of the polarization . We then discuss the electric polarization of atoms , molecules , and crystals in static ...
Page 161
Thus E3 = 0 for induced polarization on simple cubic , body - centered cubic , and face - centered cubic lattices , as well as for an isotropic distribution . Later , in considering the ferroelectric properties of barium titanate ( Fig ...
Thus E3 = 0 for induced polarization on simple cubic , body - centered cubic , and face - centered cubic lattices , as well as for an isotropic distribution . Later , in considering the ferroelectric properties of barium titanate ( Fig ...
Page 188
The spontaneous polarization as a function of temperature is shown in Fig . 8.4 . It is found by x - ray methods that the crystal structure becomes slightly deformed in the direction of the spontaneous 4.03 c - spacing 4.02 4.01 Cell ...
The spontaneous polarization as a function of temperature is shown in Fig . 8.4 . It is found by x - ray methods that the crystal structure becomes slightly deformed in the direction of the spontaneous 4.03 c - spacing 4.02 4.01 Cell ...
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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