Introduction to Solid State Physicsproblems after each chapter |
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Page 246
eikr In the approximation that the conduction electrons are entirely free we may take their wave functions to have the form ( 10.30 ) y We must do two things to this function before it can be an acceptable solution to the problem .
eikr In the approximation that the conduction electrons are entirely free we may take their wave functions to have the form ( 10.30 ) y We must do two things to this function before it can be an acceptable solution to the problem .
Page 284
WAVE FUNCTIONS FOR ZERO WAVE VECTOR It may appear to the reader that there is a certain inconsistency between the ... wave vector in approximately the same way as for a free electron while at the same time the wave function may be quite ...
WAVE FUNCTIONS FOR ZERO WAVE VECTOR It may appear to the reader that there is a certain inconsistency between the ... wave vector in approximately the same way as for a free electron while at the same time the wave function may be quite ...
Page 287
The wave function of lowest state in the conduction ( 38 ) band of metallic sodium determined by solving ( 11.32 ) is shown in Fig . 11.11 . It may be noted that the function is practically constant over 90 percent of the atomic volume ...
The wave function of lowest state in the conduction ( 38 ) band of metallic sodium determined by solving ( 11.32 ) is shown in Fig . 11.11 . It may be noted that the function is practically constant over 90 percent of the atomic volume ...
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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