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

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Page 259

motion can , however , be restricted effectively by pinning the

aid of their interactions with crystal lattice defects . Therefore , only a type II

superconductor with effectively pinned

applications .

motion can , however , be restricted effectively by pinning the

**flux**lines with theaid of their interactions with crystal lattice defects . Therefore , only a type II

superconductor with effectively pinned

**flux**lines is useful for technicalapplications .

Page 260

Herbert Herman. magnetic hardening of a superconductor and a ferromagnet

have been pointed out by Haasen ( 1969 , 1970 ) . Since the shear modulus C66

for all planes containing the directions of the

Herbert Herman. magnetic hardening of a superconductor and a ferromagnet

have been pointed out by Haasen ( 1969 , 1970 ) . Since the shear modulus C66

for all planes containing the directions of the

**flux**lines is much smaller than the ...Page 263

The crucial proposition of Eq . ( 28 ) is that the center of the specimen must be

free of

can ...

The crucial proposition of Eq . ( 28 ) is that the center of the specimen must be

free of

**flux**. Kim et al . ( 1962 , 1963 ) avoided this restriction by measuring the**flux**through a thin superconducting tube as well as the field inside . The problemcan ...

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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