Introduction to Solid State Physicsproblems after each chapter |
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Page 4
As we shall see , this requirement puts restrictions on the allowed rotations and on the translations compatible with a ... We also wish to study lattices which are invariant under more general conditions : under a rotation about a ...
As we shall see , this requirement puts restrictions on the allowed rotations and on the translations compatible with a ... We also wish to study lattices which are invariant under more general conditions : under a rotation about a ...
Page 17
We discuss first the symmetry elements associated with the three - dimensional crystal point groups : Rotation axes . One- , two- , three- , four- , and six - fold rotation axes are permissible , corresponding to rotations by 360 ° ...
We discuss first the symmetry elements associated with the three - dimensional crystal point groups : Rotation axes . One- , two- , three- , four- , and six - fold rotation axes are permissible , corresponding to rotations by 360 ° ...
Page 18
т m 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 ...
т m 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 ...
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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