Introduction to Solid State Physicsproblems after each chapter |
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Page 157
7 Dielectric Properties In this chapter we discuss first the relationship between the applied electric field and the local electric field acting on an atom . The interaction of the local field with the atom determines the polarization ...
7 Dielectric Properties In this chapter we discuss first the relationship between the applied electric field and the local electric field acting on an atom . The interaction of the local field with the atom determines the polarization ...
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 ...
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 ...
Page 236
If there were no friction in the electron system — that is , if the relaxation time were infinitely long — the conduction electrons would accelerate without limit in a constant applied electric field . The equation of motion ( 10.5 ) eE ...
If there were no friction in the electron system — that is , if the relaxation time were infinitely long — the conduction electrons would accelerate without limit in a constant applied electric field . The equation of motion ( 10.5 ) eE ...
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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