Introduction to Solid State Physicsproblems after each chapter |
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Page 3
The general parallelogram defined by primitive a , b forms a primitive cell , which is a type of unit cell . We shall later discuss unit cells in detail , but it will suffice now to state that the crystal translation operations applied ...
The general parallelogram defined by primitive a , b forms a primitive cell , which is a type of unit cell . We shall later discuss unit cells in detail , but it will suffice now to state that the crystal translation operations applied ...
Page 26
1.11 by a conventional unit cell of each . The conventional cells are not always primitive , as sometimes a multiply primitive cell has a closer connection with the symmetry elements than has a primitive cell .
1.11 by a conventional unit cell of each . The conventional cells are not always primitive , as sometimes a multiply primitive cell has a closer connection with the symmetry elements than has a primitive cell .
Page 252
The occupation number of a cell is either 0 or 1. We consider now a set of g . cells having approximately the same energy E as given by ( 10.37 ) , and we let the number of electrons in the set be ng , so that of the gg cells ng are ...
The occupation number of a cell is either 0 or 1. We consider now a set of g . cells having approximately the same energy E as given by ( 10.37 ) , and we let the number of electrons in the set be ng , so that of the gg cells ng are ...
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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