Introduction to Solid State Physicsproblems after each chapter |
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Page 22
The symmetry elements of a cube are shown in detail in Fig . 1.9 . The inversion
element is not indicated . The reader will benefit by identifying the elements of the
point group m3m shown in Fig . 1.7 with those shown in Fig . 1.9 . In interpreting ...
The symmetry elements of a cube are shown in detail in Fig . 1.9 . The inversion
element is not indicated . The reader will benefit by identifying the elements of the
point group m3m shown in Fig . 1.7 with those shown in Fig . 1.9 . In interpreting ...
Page 33
The operation of centers of symmetry at the corners of the unit cell shown in Fig .
1.20a call forth other inversion centers , and a complete plan of a unit of the
space group PT is shown in Fig . 1.20b . There are thirteen monoclinic space
groups ...
The operation of centers of symmetry at the corners of the unit cell shown in Fig .
1.20a call forth other inversion centers , and a complete plan of a unit of the
space group PT is shown in Fig . 1.20b . There are thirteen monoclinic space
groups ...
Page 445
The conditions are illustrated by Fig . ... T which is concave downwards , as
shown in Fig . 15.33 for magnetite . Here x is Fig . 15.32 . Spin arrangements
charthe susceptibility . acterizing ferromagnetism , antiferroThe Néel theory
accounts in a ...
The conditions are illustrated by Fig . ... T which is concave downwards , as
shown in Fig . 15.33 for magnetite . Here x is Fig . 15.32 . Spin arrangements
charthe susceptibility . acterizing ferromagnetism , antiferroThe Néel theory
accounts in a ...
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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