Treatise on Materials Science and Technology, Volume 2 |
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Page 259
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 II
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 II
superconductor with effectively pinned flux lines is useful for technical
applications .
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 flux lines is much smaller than 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 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 problem
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 problem
can ...
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Contents
Epitaxial Interfaces | 3 |
Thin Films | 15 |
Semiinfinite Overgrowths | 52 |
Copyright | |
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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