Introduction to Solid State Physicsproblems after each chapter |
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Page 273
We expect the ion cores to bear a positive charge , as V . potential energy -
aTelu12 , charge density Plane wave V EXXX k a 14 , 17 Fig . 11 . 2 . ( a )
Variation of potential energy of a conduction electron in the field of the positive
ion cores of a ...
We expect the ion cores to bear a positive charge , as V . potential energy -
aTelu12 , charge density Plane wave V EXXX k a 14 , 17 Fig . 11 . 2 . ( a )
Variation of potential energy of a conduction electron in the field of the positive
ion cores of a ...
Page 333
For simplicity the block drawings above represent the density of states as uniform
in energy . The actual density may be quite 3d far from uniform : Fig . 12 . 19
gives Fig . 12 . 18 . Distribution of electrons in the results of a calculation by the
alloy ...
For simplicity the block drawings above represent the density of states as uniform
in energy . The actual density may be quite 3d far from uniform : Fig . 12 . 19
gives Fig . 12 . 18 . Distribution of electrons in the results of a calculation by the
alloy ...
Page 481
0 x 10 - 4 g / cm3 KCl + CaCl2 Density change Δρ 0 0 . ... The change in density
as a function of divalent addition for KCI containing controlled amounts of CaCl2 .
... density to be expected if the densities of the two salts were purely additive .
0 x 10 - 4 g / cm3 KCl + CaCl2 Density change Δρ 0 0 . ... The change in density
as a function of divalent addition for KCI containing controlled amounts of CaCl2 .
... density to be expected if the densities of the two salts were purely additive .
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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