Introduction to Solid State Physicsproblems after each chapter |
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Page 9
THE FIVE TWO - DIMENSIONAL BRAVAIS LATTICES Point - Group Symmetry
Conventional Corresponding ( ' orresponding about Lattice Lattice Unit Cell Axes
System Points Oblique Parallelogram a #b , y # 90 ° Oblique 1 , 2 Primitive ...
THE FIVE TWO - DIMENSIONAL BRAVAIS LATTICES Point - Group Symmetry
Conventional Corresponding ( ' orresponding about Lattice Lattice Unit Cell Axes
System Points Oblique Parallelogram a #b , y # 90 ° Oblique 1 , 2 Primitive ...
Page 10
The pattern of symmetry elements is known as a space group , and a plan of a
unit of the complete space group p2 ( short symbol ) is shown in Fig . 1.6b . A
space group is a repetitive pattern of symmetry elements . It is not a crystal
structure .
The pattern of symmetry elements is known as a space group , and a plan of a
unit of the complete space group p2 ( short symbol ) is shown in Fig . 1.6b . A
space group is a repetitive pattern of symmetry elements . It is not a crystal
structure .
Page 30
The symbols which denote the several types of symmetry planes are shown in
Table 1.7 . The notation in the last column is explained in the next section .
TABLE 1.6 . SYMBOLS OF SYMMETRY Axes Symbol Symmetry Axis Graphical
Symbol ...
The symbols which denote the several types of symmetry planes are shown in
Table 1.7 . The notation in the last column is explained in the next section .
TABLE 1.6 . SYMBOLS OF SYMMETRY Axes Symbol Symmetry Axis Graphical
Symbol ...
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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