## Introduction to Solid State Physics |

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Page 28

W . L . Bragg , The crystalline state , Vol . I . , G . Bell and Sons , Ltd . ,

1933 . M . J . Buerger , X - ray crystallography , John Wiley & Sons , New York ,

1942 . C . W . Bunn , Chemical crystallography , Clarendon Press , Oxford , 1945 .

W . L . Bragg , The crystalline state , Vol . I . , G . Bell and Sons , Ltd . ,

**London**,1933 . M . J . Buerger , X - ray crystallography , John Wiley & Sons , New York ,

1942 . C . W . Bunn , Chemical crystallography , Clarendon Press , Oxford , 1945 .

Page 213

F . and H .

abandoned , 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

.

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

.

Page 219

The effect of domain structure on the magnetic susceptibility of a sphere in the

region of field intensities H . < H < H . may be discussed ; the device of a fictitious

“ intermediate state ” introduced by Peierls22 and by

...

The effect of domain structure on the magnetic susceptibility of a sphere in the

region of field intensities H . < H < H . may be discussed ; the device of a fictitious

“ intermediate state ” introduced by Peierls22 and by

**London**to describe the bulk...

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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