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

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Page 77

Furthermore , in order to comply with energy minimization , the redistributed

dislocations must form symmetrical arrangements which require them to be

equally divided among the so - called subinterfaces and to be evenly

each .

Furthermore , in order to comply with energy minimization , the redistributed

dislocations must form symmetrical arrangements which require them to be

equally divided among the so - called subinterfaces and to be evenly

**spaced**ineach .

Page 271

... give a maximal effect . Similarly , the

roughly equal to the

flux lines in contact with the obstacles without straining the flux line lattice (

Friedel et al ...

... give a maximal effect . Similarly , the

**spacing**of the obstacles should beroughly equal to the

**spacing**of the flux lines in order to maximize the number offlux lines in contact with the obstacles without straining the flux line lattice (

Friedel et al ...

Page 333

The strain perpendicular to the surface εt is given by et = ( Ad + ) / do ( 23 ) where

dot is the lattice

the lattice

The strain perpendicular to the surface εt is given by et = ( Ad + ) / do ( 23 ) where

dot is the lattice

**spacing**in the unstrained film , and Ad - is the difference betweenthe lattice

**spacing**in the strained and in the unstrained condition . It was found ...### 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