## Introduction to Solid State Physics |

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Page 23

11 ) sin MT dr * = f * u ( a ) sin war de O ur for the atomic scattering

ratio of the ... Tables of atomic scattering

Thomas - Fermi methods have been published . The results for sodium are

plotted ...

11 ) sin MT dr * = f * u ( a ) sin war de O ur for the atomic scattering

**factor**. It is theratio of the ... Tables of atomic scattering

**factors**calculated by the Hartree andThomas - Fermi methods have been published . The results for sodium are

plotted ...

Page 91

The constant N is known as the depolarization

demagnetization

exceptionally important in the field of magnetism . Values of N are plotted in Fig .

6 .

The constant N is known as the depolarization

**factor**or , more commonly , as thedemagnetization

**factor**, and its value depends on the axial ratio . It isexceptionally important in the field of magnetism . Values of N are plotted in Fig .

6 .

Page 110

w tano , 47 where the loss angle or power

! €1 . The Q

average energy loss per radian which in the dielectric case reduces to Q = - Eico

...

w tano , 47 where the loss angle or power

**factor**is defined as ( 6 . 48 ) tan 8 = 62! €1 . The Q

**factor**of a systein is defined as maximum stored energy ( 6 . 49 )average energy loss per radian which in the dielectric case reduces to Q = - Eico

...

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### Contents

LATTICE ENERGY OF IONIC CRYSTALS | 29 |

ELASTIC CONSTANTS OF CRYSTALS | 43 |

LATTICE VIBRATIONS | 60 |

Copyright | |

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alloy applied approximation atoms axes axis band boundary calculated cell chapter charge chloride condition conductivity consider constant crystal cubic defined dependence determined dielectric diffusion direction discussed dislocations displacement distance distribution domains effect elastic electric electron energy equal equation equilibrium example excitation experimental expression factor field force frequency function given gives heat holes interaction ionic ions lattice levels London magnetic magnetic field material mean measurements mechanism metals method molecules motion negative neighbor normal observed obtained parallel particles Phys physical plane polarization positive possible potential problem properties quantum range reference reflection region relation resistivity result room temperature scattering Show shown in Fig sodium solids space specimen stress structure suppose Table temperature theory thermal tion transition unit usually vacancy values volume wave zero