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
Since the shear modulus C66 for all planes containing the directions of the flux
lines is much smaller than the others near ... shown ( Thorel and Simon , 1971 )
that the perfection of the flux line lattice is astonishingly good even during flux
flow .
Since the shear modulus C66 for all planes containing the directions of the flux
lines is much smaller than the others near ... shown ( Thorel and Simon , 1971 )
that the perfection of the flux line lattice is astonishingly good even during flux
flow .
Page 266
the interactions of flux lines with single defects are comparatively small . Labusch
' s theory accounts thoroughly for the finite stiffness of the fluxons as well as their
strong coupling to the flux line lattice , problems that could be approached ...
the interactions of flux lines with single defects are comparatively small . Labusch
' s theory accounts thoroughly for the finite stiffness of the fluxons as well as their
strong coupling to the flux line lattice , problems that could be approached ...
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Contents
Epitaxial Interfaces | 3 |
Thin Films | 15 |
Semiinfinite Overgrowths | 52 |
Copyright | |
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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