Introduction to Solid State Physicsproblems after each chapter |
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Page 18
Rotation axis : X Rotation - inversion axis : X X Rotation axis with mirror plane
normal to it : X / m or Rotation axis with diad axis ( axes ) normal to it : X2 Rotation
axis with mirror plane ( planes ) parallel to it : Xm Rotation - inversion axis with ...
Rotation axis : X Rotation - inversion axis : X X Rotation axis with mirror plane
normal to it : X / m or Rotation axis with diad axis ( axes ) normal to it : X2 Rotation
axis with mirror plane ( planes ) parallel to it : Xm Rotation - inversion axis with ...
Page 467
At these frequencies hw >> kTc , and electrons are probably raised out of
superconducting states by radiation , thus explaining the “ normal ” behavior of
superconductors with respect to reflection of infrared radiation . 18 The transition
between ...
At these frequencies hw >> kTc , and electrons are probably raised out of
superconducting states by radiation , thus explaining the “ normal ” behavior of
superconductors with respect to reflection of infrared radiation . 18 The transition
between ...
Page 471
The field Hi will exceed the critical field Hc ( as determined from measurements
on a long wire in an axial field ) when ( 16.48 ) H > Hc 3 When this situation
occurs we can avoid having the whole sphere become normal by having the
material ...
The field Hi will exceed the critical field Hc ( as determined from measurements
on a long wire in an axial field ) when ( 16.48 ) H > Hc 3 When this situation
occurs we can avoid having the whole sphere become normal by having the
material ...
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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 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