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

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Page 57

When adapted for the present

to having c / p < c / 2t ( 5.17 ) C. Ball's Modelt 1. MODEL u * = μτ A model which

achieves appreciable simplification of the calculations and greater accuracy of ...

When adapted for the present

**considerations**, " small ” misfit would be equivalentto having c / p < c / 2t ( 5.17 ) C. Ball's Modelt 1. MODEL u * = μτ A model which

achieves appreciable simplification of the calculations and greater accuracy of ...

Page 70

By the foregoing

1 + ē ) 2 ( 6.4 ) with respect to ē also ... also that the

are now applied to the case where the average film strains do not vanish and ...

By the foregoing

**consideration**, the minimization ( Ball , 1970 ) of Er = Ep + 2EM (1 + ē ) 2 ( 6.4 ) with respect to ē also ... also that the

**considerations**of Section Vare now applied to the case where the average film strains do not vanish and ...

Page 82

FORCE

dislocation and on interfaces of dislocations allows one to make some

predictions regarding the stability of the dislocation arrangements . Note that the

diffusion induced ...

FORCE

**CONSIDERATIONS**Knowledge of the forces acting on a singledislocation and on interfaces of dislocations allows one to make some

predictions regarding the stability of the dislocation arrangements . Note that the

diffusion induced ...

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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