Introduction to Solid State Physicsproblems after each chapter |
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Page 18
All the points shown can be obtained from any one of them by application of the several symmetry operations . ... Starting with the point 1 , we can obtain the points 3 , 5 , and 7 by applying successive rotations of 29/4 .
All the points shown can be obtained from any one of them by application of the several symmetry operations . ... Starting with the point 1 , we can obtain the points 3 , 5 , and 7 by applying successive rotations of 29/4 .
Page 356
We may obtain a general impression of the impurity levels by using an average value of the anisotropic effective masses : we ... The values are obtained largely by thermal considerations to be 3 J. M. Luttinger and W. Kohn , Phys . Rev.
We may obtain a general impression of the impurity levels by using an average value of the anisotropic effective masses : we ... The values are obtained largely by thermal considerations to be 3 J. M. Luttinger and W. Kohn , Phys . Rev.
Page 362
We discuss here results obtained by Conwell and Debyes on n - type germanium . These results will convey an impression of the kind of information which can be obtained from a systematic analysis of conductivity and Hall data .
We discuss here results obtained by Conwell and Debyes on n - type germanium . These results will convey an impression of the kind of information which can be obtained from a systematic analysis of conductivity and Hall data .
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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