## Introduction to Solid State Physicsproblems after each chapter |

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Page 326

Jones pointed out that the observed limit of the a phase ( fcc ) occurs very close

to the electron

contact with the Brillouin zone surface for the foc lattice . The observed electron ...

Jones pointed out that the observed limit of the a phase ( fcc ) occurs very close

to the electron

**concentration**of 1 . 36 for which the inscribed Fermi sphere makescontact with the Brillouin zone surface for the foc lattice . The observed electron ...

Page 358

As the lowest impurity

impurity atoms per cm " , it is evident we may expect to be able ... Impurities with

no effect on the carrier

As the lowest impurity

**concentrations**attained at present are of the order of 1012impurity atoms per cm " , it is evident we may expect to be able ... Impurities with

no effect on the carrier

**concentration**are probably present in higher proportions .Page 362

where x = 6e dkT / e . In these equations Ne is the

donors ( or acceptors ) , and 2d is the average distance between ionized donor

neighbors . The effect of impurity scattering in reducing the mobility is shown in

Fig . 13 .

where x = 6e dkT / e . In these equations Ne is the

**concentration**of ionizeddonors ( or acceptors ) , and 2d is the average distance between ionized donor

neighbors . The effect of impurity scattering in reducing the mobility is shown in

Fig . 13 .

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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