Introduction to Solid State Physicsproblems after each chapter |
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We give in this chapter an introductory discussion of the essential symmetry properties of crystal structures . It is impossible to give a full discussion here ; the interested reader is referred to the specialized textbooks listed at ...
We give in this chapter an introductory discussion of the essential symmetry properties of crystal structures . It is impossible to give a full discussion here ; the interested reader is referred to the specialized textbooks listed at ...
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 241
The mobility is a particularly useful quantity in dealing with semiconductors , Chapter 13 . We have quoted ( but not yet derived ) the value 1.6 X 108 cm / sec for the intrinsic velocity of the conduction electrons in copper .
The mobility is a particularly useful quantity in dealing with semiconductors , Chapter 13 . We have quoted ( but not yet derived ) the value 1.6 X 108 cm / sec for the intrinsic velocity of the conduction electrons in copper .
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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