## Introduction to Solid State Physics |

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Page 134

DERIVATION OF THE LANGEVIN DIAMAGNETISM EQUATION The usual

derivation employs the Larmor theorem , which states that for an atom in a

magnetic field the

possible ...

DERIVATION OF THE LANGEVIN DIAMAGNETISM EQUATION The usual

derivation employs the Larmor theorem , which states that for an atom in a

magnetic field the

**motion**of the electrons is , to the first order in H , the same as apossible ...

Page 181

The magnetization of the crystal “ sees ” the crystal lattice through the agency of

the orbital

means of the spin orbit coupling , and the orbital

The magnetization of the crystal “ sees ” the crystal lattice through the agency of

the orbital

**motion**of the electrons ; the spin interacts with the orbital**motion**bymeans of the spin orbit coupling , and the orbital

**motion**in turn interacts with the ...Page 305

The

Parker . The nature of their results is exhibited in Fig . 16 . 7b . The specimen

consisted of a bicrystal of zinc having an orientation difference of 2° . Fig . 16 . 7a

.

The

**motion**has been demonstrated in a beautiful experiment by Washburn andParker . The nature of their results is exhibited in Fig . 16 . 7b . The specimen

consisted of a bicrystal of zinc having an orientation difference of 2° . Fig . 16 . 7a

.

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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