## Introduction to Solid State Physics |

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When all the atoms are identical we have , from ( 1 . 15 ) , F ( hkl ) = fs , where S is

called the geometrical

; + lw ; ) A body - centered cubic

When all the atoms are identical we have , from ( 1 . 15 ) , F ( hkl ) = fs , where S is

called the geometrical

**structure**factor and is given by ( 1 . 17 ) S = ei27 ( hu ; + kv; + lw ; ) A body - centered cubic

**structure**of identical atoms has atoms at 000 ...Page 35

747558 which has been worked out for the sodium chloride

Ewald method . The Ewald method is derived and discussed in Appendix B .

Values of Madelung constants for many different crystal

by ...

747558 which has been worked out for the sodium chloride

**structure**by theEwald method . The Ewald method is derived and discussed in Appendix B .

Values of Madelung constants for many different crystal

**structures**are tabulatedby ...

Page 116

The

centers , and a Ti4 + ion at the body center . Below the Curie temperature the

The

**structure**is cubic , with Ba2 + ions at the cube corners , 02 - ions at the facecenters , and a Ti4 + ion at the body center . Below the Curie temperature the

**structure**is slightly deformed with respect to that described here . The prototype ...### What people are saying - Write a review

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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