Introduction to Solid State Physicsproblems after each chapter |
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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 236
The electric current density j is defined as the electric charge transported through unit area in unit time . The net number of electrons passing through a unit area in unit time is Nvp , where N is the number of electrons per unit ...
The electric current density j is defined as the electric charge transported through unit area in unit time . The net number of electrons passing through a unit area in unit time is Nvp , where N is the number of electrons per unit ...
Page 313
The volume of the primitive cell is ( 12.3 ) V = a b Xc = ta ' ; we see that this is correct because the unit cube of volume a ' contains two lattice points . The primitive translations a * , b * , c * of the reciprocal lattice are ...
The volume of the primitive cell is ( 12.3 ) V = a b Xc = ta ' ; we see that this is correct because the unit cube of volume a ' contains two lattice points . The primitive translations a * , b * , c * of the reciprocal lattice 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