## 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 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 ...

Page 515

Conduction band It is convenient to

entirely Trap levels trapped and a fraction of the elec ... We shall

very simple models ; for a

and more ...

Conduction band It is convenient to

**discuss**models in which the holes areentirely Trap levels trapped and a fraction of the elec ... We shall

**discuss**onlyvery simple models ; for a

**discussion**of the proValence band perties of detailedand more ...

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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 axes 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 magnetic field 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