## Introduction to Solid State Physics |

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Page 99

19 ) P = 2wo % a3 \ m ' which gives directly the Born

wo ? a ? Im This exhibits the connection of Ae with the residual ray frequency wo

. Values of Ae calculated by using this

19 ) P = 2wo % a3 \ m ' which gives directly the Born

**equation**2me ? / 1 ( 6 . 20 )wo ? a ? Im This exhibits the connection of Ae with the residual ray frequency wo

. Values of Ae calculated by using this

**equation**are in fairly good agreement ...Page 155

MACROSCOPIC

process in terms of the magnetic ... M for the magnetization ( magnetic moment /

volume ) and J for the angular momentum density , the classical

MACROSCOPIC

**EQUATIONS**It is sometimes useful to consider the resonanceprocess in terms of the magnetic ... M for the magnetization ( magnetic moment /

volume ) and J for the angular momentum density , the classical

**equation**of ...Page 213

F . and H . London 16 therefore suggested that the acceleration

abandoned , and that we should take instead as the fundamental

22 ) c curl Aj = - H , which is postulated to replace Ohm ' s law in superconductors

.

F . and H . London 16 therefore suggested that the acceleration

**equation**beabandoned , and that we should take instead as the fundamental

**equation**( 11 .22 ) c curl Aj = - H , which is postulated to replace Ohm ' s law in superconductors

.

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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