## Introduction to Solid State Physicsproblems after each chapter |

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Page 159

The constant N is known as the depolarization

the demagnetization

0.4 0.2 0 5 cla Fig . 7.2 . Demagnetization

The constant N is known as the depolarization

**factor**; it is precisely the same asthe demagnetization

**factor**, and its value depends on the axial 1.0 0.8 0.6 N / 400.4 0.2 0 5 cla Fig . 7.2 . Demagnetization

**factor**N parallel to the figure axis of ...Page 237

We expect the charge transported to be proportional to the charge density Ne ;

the

proportional to e and inversely proportional to the mass m ; the time t describes

the free ...

We expect the charge transported to be proportional to the charge density Ne ;

the

**factor**e / m enters because the acceleration in a given electric field isproportional to e and inversely proportional to the mass m ; the time t describes

the free ...

Page 359

In writing ( 13.26 ) we have omitted in the interest of simplicity a

often is seen in front of the exponential . The

account the fact that the energy of a spindegenerate donor level occupied by two

...

In writing ( 13.26 ) we have omitted in the interest of simplicity a

**factor**of whichoften is seen in front of the exponential . The

**factor**arises when one takes intoaccount the fact that the energy of a spindegenerate donor level occupied by two

...

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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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### 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