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

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Page 159

The correct procedure is to average for a sufficient number of small crystals with

N

mathematical procedures to perform this we choose for this discussion the use of

the long ...

The correct procedure is to average for a sufficient number of small crystals with

N

**lattice**sites containing an average of No defects . Among the variousmathematical procedures to perform this we choose for this discussion the use of

the long ...

Page 160

However if a homogeneous average

Syk , 1 = 0 ( IV . 12 ) must be fulfilled for every l . This says the average distance

between two atoms in a counting distance R4 is exactly R , " . The individual svu ,

i ...

However if a homogeneous average

**lattice**exists , the condition Ec , cu Bum , iSyk , 1 = 0 ( IV . 12 ) must be fulfilled for every l . This says the average distance

between two atoms in a counting distance R4 is exactly R , " . The individual svu ,

i ...

Page 259

motion can , however , be restricted effectively by pinning the flux lines with the

aid of their interactions with crystal

superconductor with effectively pinned flux lines is useful for technical

applications .

motion can , however , be restricted effectively by pinning the flux lines with the

aid of their interactions with crystal

**lattice**defects . Therefore , only a type IIsuperconductor with effectively pinned flux lines is useful for technical

applications .

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### Contents

Epitaxial Interfaces | 3 |

Thin Films | 15 |

Semiinfinite Overgrowths | 52 |

Copyright | |

10 other sections not shown

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### Common terms and phrases

angle anisotropy approximation assumed atoms average axis c-site calculated cations coherent compounds concentration condition considerations constants contribution corresponding crystal curve decreases defect density dependence determined diffusion direction discussed dislocations displacement effect elastic elastic scattering electron energy equation et al experimental experiments factor field flux flux lines follows force function garnets given gives important impurity increases interaction interface ions lattice limit magnetic materials measured Merwe metal method misfit mode neutron normal observed obtained optical parameter phase phonon Phys plane position potential present processes properties range reference region 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 wave X-ray