Introduction to Solid State Physicsproblems after each chapter |
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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 ...
Page 440
... a twosublattice model : first , with the ap( b ) plied magnetic field perpendicular to Fig . 15.28 . Calculation of ( a ) per- the axis of the spins ; and , second , pendicular and ( b ) parallel suscepti- with the field parallel to ...
... a twosublattice model : first , with the ap( b ) plied magnetic field perpendicular to Fig . 15.28 . Calculation of ( a ) per- the axis of the spins ; and , second , pendicular and ( b ) parallel suscepti- with the field parallel to ...
Page 441
Molar magnetic susceptibility of manganese fluoride , MnF2 , parallel and perpendicular to the c axis of the crystal . ( After Griffel and Stout . ) Recent measurements suggest x1 is horizontal below Tc . In the parallel orientation ...
Molar magnetic susceptibility of manganese fluoride , MnF2 , parallel and perpendicular to the c axis of the crystal . ( After Griffel and Stout . ) Recent measurements suggest x1 is horizontal below Tc . In the parallel orientation ...
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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