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 187
... which is parallel to a cube edge above 0 ° C , becomes parallel to a face
diagonal below 0 ° C and parallel to a body diagonal below –80 ° C , as the
ratios of the P , at the transition temperatures are approximately 1 : 1/22 : 1 / 3 % .
... which is parallel to a cube edge above 0 ° C , becomes parallel to a face
diagonal below 0 ° C and parallel to a body diagonal below –80 ° C , as the
ratios of the P , at the transition temperatures are approximately 1 : 1/22 : 1 / 3 % .
Page 441
Molar magnetic susceptibility of manganese fluoride , MnF2 , parallel and
perpendicular to the c axis of the crystal . ( After Griffel and Stout . ) In the parallel
orientation ( Fig . 15.28b ) the susceptibility at T = 0 ° K is zero : ( 15.64 ) xi ( 0 ) =
0 ; the ...
Molar magnetic susceptibility of manganese fluoride , MnF2 , parallel and
perpendicular to the c axis of the crystal . ( After Griffel and Stout . ) In the parallel
orientation ( Fig . 15.28b ) the susceptibility at T = 0 ° K is zero : ( 15.64 ) xi ( 0 ) =
0 ; the ...
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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