Introduction to Solid State Physicsproblems after each chapter |
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Page 56
All three of the above methods are employed , sometimes with modifications , in
current research . The Laue method is convenient for the rapid determination of
crystal orientation and symmetry and also for studying the extent of crystalline ...
All three of the above methods are employed , sometimes with modifications , in
current research . The Laue method is convenient for the rapid determination of
crystal orientation and symmetry and also for studying the extent of crystalline ...
Page 59
POWDER METHOD In the powder method illustrated in Fig . 2 . 14 the incident
monochromatic radiation strikes a finely powdered specimen or a finegrained
polycrystalline specimen contained in a thin - walled capillary tube . Diffracted
rays ...
POWDER METHOD In the powder method illustrated in Fig . 2 . 14 the incident
monochromatic radiation strikes a finely powdered specimen or a finegrained
polycrystalline specimen contained in a thin - walled capillary tube . Diffracted
rays ...
Page 285
Wigner and Seitz have developed a simple and fairly accurate method of
calculating uo ( r ) if the field of the free ion is known . We discuss their method
below . There have been many developments in the calculation of wave functions
in ...
Wigner and Seitz have developed a simple and fairly accurate method of
calculating uo ( r ) if the field of the free ion is known . We discuss their method
below . There have been many developments in the calculation of wave functions
in ...
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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 neighbor normal observed obtained parallel particles Phys physics plane polarization positive possible potential 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