Introduction to Solid State Physicsproblems after each chapter |
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Page 284
In the last chapter the important result of the free electron model was the relation 111.25 ) E ( h / 2m ) k . We can broaden the scope of the treatment by observing that the really important part of the result is the quadratic ...
In the last chapter the important result of the free electron model was the relation 111.25 ) E ( h / 2m ) k . We can broaden the scope of the treatment by observing that the really important part of the result is the quadratic ...
Page 306
Thus it is the value of the wave number which is important for the energy discontinuities . In three dimensions the wave vector k plays the same role , as we see from the Bragg equation ( 2.1 ) or ( 2.12 ) . The equation determining the ...
Thus it is the value of the wave number which is important for the energy discontinuities . In three dimensions the wave vector k plays the same role , as we see from the Bragg equation ( 2.1 ) or ( 2.12 ) . The equation determining the ...
Page 383
The junction devices are in many respects easiest to discuss quantitatively , but the barrier rectifier and point contact transistor are of practical and historical importance . Thus , the development of the high - back - voltage ...
The junction devices are in many respects easiest to discuss quantitatively , but the barrier rectifier and point contact transistor are of practical and historical importance . Thus , the development of the high - back - voltage ...
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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