Introduction to Solid State Physicsproblems after each chapter |
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Page 35
SIMPLE CRYSTAL STRUCTURES We discuss briefly a small number of simple
crystal structures of general interest , including the hexagonal close ... The
perovskite structure is discussed in Chapter 7 and the spinel structure in Chapter
15 .
SIMPLE CRYSTAL STRUCTURES We discuss briefly a small number of simple
crystal structures of general interest , including the hexagonal close ... The
perovskite structure is discussed in Chapter 7 and the spinel structure in Chapter
15 .
Page 36
DIAMOND STRUCTURE The space lattice of diamond is face - centered cubic
with a basis of two atoms at 000 ; } } associated with each lattice point , as shown
in Fig . 1.27 . The tetrahedral bonding of the diamond structure is exhibited in Fig
.
DIAMOND STRUCTURE The space lattice of diamond is face - centered cubic
with a basis of two atoms at 000 ; } } associated with each lattice point , as shown
in Fig . 1.27 . The tetrahedral bonding of the diamond structure is exhibited in Fig
.
Page 185
The third group of ferroelectrics consists of ionic crystals with crystal structures
closely related to the perovskite and ilmenite structures . The perovskite structure
is the simplest crystal structure ( Figs . 8.1 Ba Ti Oxygen Fig . 8.1 . The perovskite
...
The third group of ferroelectrics consists of ionic crystals with crystal structures
closely related to the perovskite and ilmenite structures . The perovskite structure
is the simplest crystal structure ( Figs . 8.1 Ba Ti Oxygen Fig . 8.1 . The perovskite
...
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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