## Introduction to Solid State Physics |

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Page 8

We now enumerate the fundamental macroscopic symmetry elements : rotation

Rotation

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 canbe ...

Page 9

A crystal has a rotation - reflection

combined rotation and reflection in a plane perpendicular to the

Crystals can possess one - , two - , three - , four - , or six - fold rotation - reflection

A crystal has a rotation - reflection

**axis**if it is brought into self - coincidence bycombined 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

preferred

...

The anisotropy energy tends to make the magnetization of a domain line up

along certain crystallographic

**axes**. The**axes**thus favored are known aspreferred

**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