## Introduction to Solid State Physicsproblems after each chapter |

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Page 35

SIMPLE CRYSTAL STRUCTURES We discuss briefly a small number of simple

crystal structures of general interest , including the hexagonal close - packed ,

diamond ,

SIMPLE CRYSTAL STRUCTURES We discuss briefly a small number of simple

crystal structures of general interest , including the hexagonal close - packed ,

diamond ,

**cubic**zinc sulfide , sodium chloride , cesium chloride , and fluorite ...Page 42

Find the space group of the

the maximum proportion of the available volume which may be filled by hard

spheres arranged in various structures is Simple

Find the space group of the

**cubic**ZnS ( zinc blende ) structure . 1 . 5 . Show thatthe maximum proportion of the available volume which may be filled by hard

spheres arranged in various structures is Simple

**cubic**Body - centered**cubic**...Page 161

The proof we have given for the vanishing of Ez actually obtains for all cases in

which the environment of the reference point is

parallel . Thus Ez = 0 for induced polarization on simple

The proof we have given for the vanishing of Ez actually obtains for all cases in

which the environment of the reference point is

**cubic**, as long as the dipoles areparallel . Thus Ez = 0 for induced polarization on simple

**cubic**, body - centered ...### What people are saying - Write a review

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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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### Common terms and phrases

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 mass material measurements metals method motion normal observed obtained parallel particles Phys physics plane polarization positive possible potential present 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