Introduction to Solid State Physicsproblems after each chapter |
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Page 273
2 ( a ) we have indicated the general nature of the variation of the electrostatic
potential energy of a conduction electron in the field of the positive ion cores of a
monatomic linear lattice . We expect the ion cores to bear a positive charge , as V
...
2 ( a ) we have indicated the general nature of the variation of the electrostatic
potential energy of a conduction electron in the field of the positive ion cores of a
monatomic linear lattice . We expect the ion cores to bear a positive charge , as V
...
Page 388
Over most of the potential curve of the barrier layer eV » kT , so that the density of
conduction electrons may be supposed to be zero in this region for the purpose
of estimating the form of the potential variation . Now ( 14 . 1 ) div D = 47p , or ...
Over most of the potential curve of the barrier layer eV » kT , so that the density of
conduction electrons may be supposed to be zero in this region for the purpose
of estimating the form of the potential variation . Now ( 14 . 1 ) div D = 47p , or ...
Page 571
The problem is to calculate the electrostatic potential experienced by one ion in
the presence of all the other ions in the crystal . ... We compute the total potential (
A . 1 ) y = y 1 + 42 at an ion as the sum of two distinct but related potentials .
The problem is to calculate the electrostatic potential experienced by one ion in
the presence of all the other ions in the crystal . ... We compute the total potential (
A . 1 ) y = y 1 + 42 at an ion as the sum of two distinct but related potentials .
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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 neighbor 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