## Introduction to Solid State Physics |

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Page 13

The region of space which can be reached from 0 without crossing any of the

and orientation of a crystal

...

The region of space which can be reached from 0 without crossing any of the

**planes**then satisfies the requirements for a unit ... MILLER INDICES The positionand orientation of a crystal

**plane**is determined by giving the coordinates of three...

Page 20

matical construction and may be spoken of as the reflecting

angle s makes with so , then 0 is the angle of incidence , and from the figure we

see that S = 2 sin 0 , as s and so are unit vectors . The phase difference ® is 27 /

1 ...

matical construction and may be spoken of as the reflecting

**plane**. If 20 is theangle s makes with so , then 0 is the angle of incidence , and from the figure we

see that S = 2 sin 0 , as s and so are unit vectors . The phase difference ® is 27 /

1 ...

Page 21

elementary

proportional to h / a , k / b , 1 / C . Therefore the lattice

parallel to the reflecting

scattering ...

elementary

**plane**geometry the direction cosines of the normal to ( hkl ) areproportional to h / a , k / b , 1 / C . Therefore the lattice

**planes**( hkl ) must beparallel to the reflecting

**plane**, and the diffraction maxima occur when thescattering ...

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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