Introduction to Solid State Physicsproblems after each chapter |
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Page 133
Each value has associated with it three different modes , having different and orthogonal polarization directions . There are thus a total of 3N independent lattice modes associated with N atoms , if we neglect the six degrees of ...
Each value has associated with it three different modes , having different and orthogonal polarization directions . There are thus a total of 3N independent lattice modes associated with N atoms , if we neglect the six degrees of ...
Page 529
Bowers and Melamed 14 and Kroger15 have suggested identifications of the several types of traps associated with specific emission bands in ZnS : Cu : Cl phosphors . Their identifications are based in part on the observation that all the ...
Bowers and Melamed 14 and Kroger15 have suggested identifications of the several types of traps associated with specific emission bands in ZnS : Cu : Cl phosphors . Their identifications are based in part on the observation that all the ...
Page 598
+ 0.0000030 1836.1388 + 0.0339 ( 1.3802565 + 0.0000615 ) X 10-16 erg deg - 1 Bohr magneton , HB eh / 2mc Wavelength associated with 1 ev , de Frequency associated with 1 ev , vo Wave number associated with 1 ev , ko Energy associated ...
+ 0.0000030 1836.1388 + 0.0339 ( 1.3802565 + 0.0000615 ) X 10-16 erg deg - 1 Bohr magneton , HB eh / 2mc Wavelength associated with 1 ev , de Frequency associated with 1 ev , vo Wave number associated with 1 ev , ko Energy associated ...
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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