Introduction to Solid State Physics |
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Page 8
We now enumerate the fundamental macroscopic symmetry elements : rotation
axes , reflection planes , inversion centers , and rotation - reflection axes .
Rotation axis . If a crystal possesses a rotation axis of symmetry , the crystal can
be ...
We now enumerate the fundamental macroscopic symmetry elements : rotation
axes , reflection planes , inversion centers , and rotation - reflection axes .
Rotation axis . If a crystal possesses a rotation axis of symmetry , the crystal can
be ...
Page 9
A crystal has a rotation - reflection axis if it is brought into self - coincidence by
combined rotation and reflection in a plane perpendicular to the axis of ...
Crystals can possess one - , two - , three - , four - , or six - fold rotation - reflection
axes .
A crystal has a rotation - reflection axis if it is brought into self - coincidence by
combined rotation and reflection in a plane perpendicular to the axis of ...
Crystals can possess one - , two - , three - , four - , or six - fold rotation - reflection
axes .
Page 176
The anisotropy energy tends to make the magnetization of a domain line up
along certain crystallographic axes . The axes thus favored are known as
preferred axes , or axes of easy magnetization . Such axes are well - established
...
The anisotropy energy tends to make the magnetization of a domain line up
along certain crystallographic axes . The axes thus favored are known as
preferred axes , or axes of easy magnetization . Such axes are well - established
...
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Contents
LATTICE ENERGY OF IONIC CRYSTALS | 29 |
ELASTIC CONSTANTS OF CRYSTALS | 43 |
LATTICE VIBRATIONS | 60 |
Copyright | |
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alloy applied approximation atoms axes axis band boundary calculated cell chapter charge chloride condition conductivity consider constant crystal cubic defined dependence determined dielectric diffusion direction discussed dislocations displacement distance distribution domains effect elastic electric electron energy equal equation equilibrium example excitation experimental expression factor field force frequency function given gives heat holes interaction ionic ions lattice levels London magnetic magnetic field material mean measurements mechanism metals method molecules motion negative neighbor normal observed obtained parallel particles Phys physical plane polarization positive possible potential problem properties quantum range reference reflection region relation resistivity result room temperature scattering Show shown in Fig sodium solids space specimen stress structure suppose Table temperature theory thermal tion transition unit usually vacancy values volume wave zero