## Introduction to Solid State Physicsproblems after each chapter |

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Page 262

EFFECT OF FERMI - DIRAC

CONDUCTIVITY It is a somewhat surprising fact that the introduction of the

FermiDirac

usually has little ...

EFFECT OF FERMI - DIRAC

**DISTRIBUTION**ON THE ELECTRICALCONDUCTIVITY It is a somewhat surprising fact that the introduction of the

FermiDirac

**distribution**in place of the classical Maxwell - Boltzmann**distribution**usually has little ...

Page 264

The corresponding situation with the Fermi - Dirac

. 7 . The exclusion principle has no effect on the | P ( ux , 0 ) eEt / m | P ( ug , 7 ) |

P ( uç , ) - P ( ug , 0 ) Fig . 10 . 7 . Fermi - Dirac velocity

The corresponding situation with the Fermi - Dirac

**distribution**is shown in Fig . 10. 7 . The exclusion principle has no effect on the | P ( ux , 0 ) eEt / m | P ( ug , 7 ) |

P ( uç , ) - P ( ug , 0 ) Fig . 10 . 7 . Fermi - Dirac velocity

**distribution**in one ...Page 571

The potential $ 1 is that of a structure with a Gaussian

situated at each ion site , with signs the same as those of the real ions . According

to the definition of the Madelung constant , the charge

reference ...

The potential $ 1 is that of a structure with a Gaussian

**distribution**of chargesituated at each ion site , with signs the same as those of the real ions . According

to the definition of the Madelung constant , the charge

**distribution**on thereference ...

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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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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