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

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Page 158

Herbert Herman. position vector Rio = 0. We obtain a scattering length bo of the

. The vectors sy are the distortion vectors originated by the

Herbert Herman. position vector Rio = 0. We obtain a scattering length bo of the

**defect**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 171

fore especially large for

... The contour lines have been discussed for instance by Krivoglaz ( 1969 ) and

for

fore especially large for

**defects**with appreciable volume change like interstitials .... The contour lines have been discussed for instance by Krivoglaz ( 1969 ) and

for

**defect**clusters where the same formalism can be used as shown by ...Page 172

The wavelength dependence of the

and the angular dependence of the ... used as an indication for

BeO ) , for amorphous zones ( SiO2 ) , and for point

...

The wavelength dependence of the

**defect**induced change in total cross sectionand the angular dependence of the ... used as an indication for

**defect**clusters (BeO ) , for amorphous zones ( SiO2 ) , and for point

**defects**or very small clusters...

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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