Introduction to Solid State Physicsproblems after each chapter |
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Page 36
First - layer atoms Oo Second - layer atoms + + Third - layer atoms Fig . 1 . 26 .
Modes of superposition of close - packed layers of spheres in ( a ) cubic close -
packing and ( b ) hexagonal close - packing . DIAMOND STRUCTURE The
space ...
First - layer atoms Oo Second - layer atoms + + Third - layer atoms Fig . 1 . 26 .
Modes of superposition of close - packed layers of spheres in ( a ) cubic close -
packing and ( b ) hexagonal close - packing . DIAMOND STRUCTURE The
space ...
Page 65
IONIC CRYSTALS In ionic crystals electrons are transferred from atoms of one
type to atoms of a second type , so that the crystal is made up of positive and
negative ions . The ions arrange themselves so the Coulomb attraction between
ions ...
IONIC CRYSTALS In ionic crystals electrons are transferred from atoms of one
type to atoms of a second type , so that the crystal is made up of positive and
negative ions . The ions arrange themselves so the Coulomb attraction between
ions ...
Page 274
It is useful also to look at the formation of allowed and forbidden bands in another
way , starting from the energy levels of the neutral separated atoms and watching
the changes in the levels as the charge distributions of adjacent atoms overlap ...
It is useful also to look at the formation of allowed and forbidden bands in another
way , starting from the energy levels of the neutral separated atoms and watching
the changes in the levels as the charge distributions of adjacent atoms overlap ...
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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