Introduction to Solid State Physicsproblems after each chapter |
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Page 389
The electric current density incident on the barrier from the left is then Neū . The current crossing the barrier from left to right is just this quantity times e - em kr , as this factor gives the probability that an electron will have ...
The electric current density incident on the barrier from the left is then Neū . The current crossing the barrier from left to right is just this quantity times e - em kr , as this factor gives the probability that an electron will have ...
Page 480
It is generally believed on the basis of ionic conductivity studies and density measurements that in pure alkali halides the most common lattice vacancies are Schottky defects while in pure silver halides the most common vacancies arise ...
It is generally believed on the basis of ionic conductivity studies and density measurements that in pure alkali halides the most common lattice vacancies are Schottky defects while in pure silver halides the most common vacancies arise ...
Page 554
DISLOCATION DENSITIES 2 The density of dislocations is specified by giving the number of dislocation lines that intersect a unit area in the crystal . The density ranges from 102 to 10 dislocations / cm2 in the best germanium and ...
DISLOCATION DENSITIES 2 The density of dislocations is specified by giving the number of dislocation lines that intersect a unit area in the crystal . The density ranges from 102 to 10 dislocations / cm2 in the best germanium and ...
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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 present 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