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 lattice sites containing an average of No defects . Among the various
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 various
mathematical procedures to perform this we choose for this discussion the use of
the long ...
Page 160
However if a homogeneous average lattice exists , the condition Ec , cu Bum , i
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 , i
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 ...
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 .
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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