Introduction to Solid State Physicsproblems after each chapter |
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Page 108
These features of the onedimensional problem are characteristic also of the
lattice vibration problems in two and three dimensions . We sometimes wish to
know the number of modes per unit range of k . We shall denote this quantity by
w ( k ) ...
These features of the onedimensional problem are characteristic also of the
lattice vibration problems in two and three dimensions . We sometimes wish to
know the number of modes per unit range of k . We shall denote this quantity by
w ( k ) ...
Page 180
PROBLEMS 7.1 . ( a ) Show that the expression ( 7.14 ) applied to ... In the local
field problem the cavity need not be chosen as spherical , but may be of any
shape possessing at least cubic symmetry . We may for example take the cavity
as a ...
PROBLEMS 7.1 . ( a ) Show that the expression ( 7.14 ) applied to ... In the local
field problem the cavity need not be chosen as spherical , but may be of any
shape possessing at least cubic symmetry . We may for example take the cavity
as a ...
Page 505
The problem is much like the hydrogen atom problem and the problem of donor
and acceptor levels considered in Chapter 13. The energy levels referred to the
bottom of the conduction band are given by the modified Rydberg formula En ...
The problem is much like the hydrogen atom problem and the problem of donor
and acceptor levels considered in Chapter 13. The energy levels referred to the
bottom of the conduction band are given by the modified Rydberg formula En ...
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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 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