Introduction to Solid State Physicsproblems after each chapter |
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The discussion of the symmetry of crystals in three dimensions can become rather tedious , and instead we shall treat fairly completely the theory of crystals in two dimensions , with a discussion of only a few important examples of ...
The discussion of the symmetry of crystals in three dimensions can become rather tedious , and instead we shall treat fairly completely the theory of crystals in two dimensions , with a discussion of only a few important examples of ...
Page 103
5 Lattice Vibrations In this chapter we discuss the elastic vibrations of crystals . We extend the discussion of the preceding chapter to the short wavelength range , where the wavelength of the lattice wave is comparable with the ...
5 Lattice Vibrations In this chapter we discuss the elastic vibrations of crystals . We extend the discussion of the preceding chapter to the short wavelength range , where the wavelength of the lattice wave is comparable with the ...
Page 176
DEBYE RELAXATION TIME Debyel has given an elegant discussion of dielectric relaxation in polar liquids and in solutions of polar molecules in non - polar solvents ; his central result is that the orientational part of the polarizability ...
DEBYE RELAXATION TIME Debyel has given an elegant discussion of dielectric relaxation in polar liquids and in solutions of polar molecules in non - polar solvents ; his central result is that the orientational part of the polarizability ...
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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