## Introduction to Solid State Physicsproblems after each chapter |

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Page 286

To satisfy these two

boundary planes of each polyhedron . ... The cubes show the unit cells in either

case . sphere is determined by the

To satisfy these two

**conditions**the normal derivative duo / an must vanish on theboundary planes of each polyhedron . ... The cubes show the unit cells in either

case . sphere is determined by the

**condition**that the volume of the s sphere be ...Page 373

... wrlw , for various relaxation times in units wt . Curves are given for both linear

polarization and circular polarization of the r - f field . It is interesting to state in

terms of the mobility the

resonance .

... wrlw , for various relaxation times in units wt . Curves are given for both linear

polarization and circular polarization of the r - f field . It is interesting to state in

terms of the mobility the

**condition**wt > 1 for the observation of cyclotronresonance .

Page 585

We note that the Bragg

also marks the boundaries on the KronigPenney model . At the boundary the

wave functions are standing waves which do not carry current . For k just above

the ...

We note that the Bragg

**condition**for reflection is also k = in / a , and this**condition**also marks the boundaries on the KronigPenney model . At the boundary the

wave functions are standing waves which do not carry current . For k just above

the ...

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