Introduction to Solid State Physicsproblems after each chapter |
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Page 299
We now consider in detail the motion of a hole in an applied electric field . We
treat the one - dimensional example illustrated by Fig . 11.15 . Initially the band is
filled except for the single vacant state F at the top of the band . An electric field E
...
We now consider in detail the motion of a hole in an applied electric field . We
treat the one - dimensional example illustrated by Fig . 11.15 . Initially the band is
filled except for the single vacant state F at the top of the band . An electric field E
...
Page 553
Motion of the boundary took place by cooperative motion of the dislocations in
the array , each dislocation moving an equal distance in its own slip plane .
Opposite top and bottom intersections at the boundary with the surface moved ...
Motion of the boundary took place by cooperative motion of the dislocations in
the array , each dislocation moving an equal distance in its own slip plane .
Opposite top and bottom intersections at the boundary with the surface moved ...
Page 559
All four of these strengthening mechanisms depend for their success upon
impeding dislocation motion . A fifth mechanism , that of removing all dislocations
from the crystal , may operate for certain fine hair - like crystals that are discussed
in ...
All four of these strengthening mechanisms depend for their success upon
impeding dislocation motion . A fifth mechanism , that of removing all dislocations
from the crystal , may operate for certain fine hair - like crystals that are discussed
in ...
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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