## Introduction to Solid State Physicsproblems after each chapter |

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Page 2

The

rather tedious , and instead we shall treat fairly completely the theory of crystals

in two dimensions , with a

structures in ...

The

**discussion**of the symmetry of crystals in three dimensions can becomerather tedious , and instead we shall treat fairly completely the theory of crystals

in two dimensions , with a

**discussion**of only a few important examples ofstructures in ...

Page 42

( a )

; explain how each symmetry element occurs . ( b ) Do the ... Show with a full

the ...

( a )

**Discuss**the symmetry elements of the two - dimensional space group p4mm; explain how each symmetry element occurs . ( b ) Do the ... Show with a full

**discussion**that the space group of the diamond structure is F41 / d32 / m . Findthe ...

Page 176

DEBYE RELAXATION TIME Debyel2 has given an elegant

dielectric relaxation in polar liquids and in solutions of polar molecules in non -

polar solvents ; his central result is that the orientational part of the polarizability

depends ...

DEBYE RELAXATION TIME Debyel2 has given an elegant

**discussion**ofdielectric relaxation in polar liquids and in solutions of polar molecules in non -

polar solvents ; his central result is that the orientational part of the polarizability

depends ...

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### Contents

DIFFRACTION OF XRAYS BY CRYSTALS | 44 |

CLASSIFICATION OF SOLIDS LATTICE ENERGY | 63 |

ELASTIC CONSTANTS OF CRYSTALS | 85 |

Copyright | |

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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 neighbor 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