## Introduction to Solid State Physics |

### From inside the book

Results 1-3 of 27

Page 13

A convenient way of choosing the unit

draw the various vectors nia + n2b + nzc and then bisect each vector with a plane

perpendicular to it . The region of space which can be reached from 0 without ...

A convenient way of choosing the unit

**cell**is to choose an origin 0 and from itdraw the various vectors nia + n2b + nzc and then bisect each vector with a plane

perpendicular to it . The region of space which can be reached from 0 without ...

Page 14

The positions of points in a unit

in which each coordinate is a fraction of the axial length , a , b , or c , in the

direction of the coordinate , with the origin taken at the corner of a unit

the ...

The positions of points in a unit

**cell**are specified in terms of lattice coordinates ,in which each coordinate is a fraction of the axial length , a , b , or c , in the

direction of the coordinate , with the origin taken at the corner of a unit

**cell**. Thusthe ...

Page 16

The unit

atom added within the prism , so that the hcp unit

DIAMOND STRUCTURE The space lattice of diamond is fcc with two atoms 000 ;

I 1 i ...

The unit

**cell**of the hcp structure is the hexagonal primitive**cell**but with an extraatom added within the prism , so that the hcp unit

**cell**contains two atoms .DIAMOND STRUCTURE The space lattice of diamond is fcc with two atoms 000 ;

I 1 i ...

### What people are saying - Write a review

We haven't found any reviews in the usual places.

### Contents

LATTICE ENERGY OF IONIC CRYSTALS | 29 |

ELASTIC CONSTANTS OF CRYSTALS | 43 |

LATTICE VIBRATIONS | 60 |

Copyright | |

13 other sections not shown

### Other editions - View all

### Common terms and phrases

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