## Treatise on Materials Science and Technology, Volume 2 |

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Page 124

... different phonon branches j . V ; ' is the polarization

phonon of branch j . My is the mass of atom y in the unit cell , R , its position

lattices : Fayn ...

... different phonon branches j . V ; ' is the polarization

**vector**of atom y for aphonon of branch j . My is the mass of atom y in the unit cell , R , its position

**vector**. The dynamical structure factor Fdyn , j is rather simple for monatomiclattices : Fayn ...

Page 158

Herbert Herman. position

defect at R , ° = 0 and new position

. The

Herbert Herman. position

**vector**Rio = 0. We obtain a scattering length bo of thedefect at R , ° = 0 and new position

**vectors**for the host lattice atoms R , = R , ° + si. The

**vectors**sy are the distortion**vectors**originated by the defect . We set s ( R ...Page 182

The equation is very evident in its dependence on concentration c , temperature ,

and interaction potential . V ( K ) has negative or positive values depending on

whether a concentration wave with wave

The equation is very evident in its dependence on concentration c , temperature ,

and interaction potential . V ( K ) has negative or positive values depending on

whether a concentration wave with wave

**vector**K is energetically favorable or ...### What people are saying - Write a review

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### Contents

Epitaxial Interfaces | 3 |

Thin Films | 15 |

Semiinfinite Overgrowths | 37 |

Copyright | |

11 other sections not shown

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### Common terms and phrases

angle anisotropy approximation assumed atoms average axis c-sites calculated cations coherent concentration condition considerations constant contribution corresponding crystal curve defect density dependence determined diffusion direction discussed dislocations displacement effect elastic elastic scattering electron energy equation et al exist experimental experiments factor field flux lines follows force function garnet given gives important increasing Inelastic Scattering interaction interface ions lattice length limit magnetic materials measured Merwe metal method misfit mode neutron normal obtained parameter phase phonon Phys plane position potential present properties range rare earth reasonable reference region relation resolution respectively sample scattering cross section shown shows single solid solution space strain stress structure substrate superconducting surface Table temperature tetrahedral theory thermal thickness transition unit values vector X-ray