Treatise on Materials Science and Technology, Volume 2 |
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Page 92
14 ) thus becomes Pzz ( 0 , x ) = [ 2u / ( 1 – 20 ) ] ( W / d ) ( B . 1 ) It has only been
possible to solve the elastic problem with this extra boundary condition , for the
unrealistic parabolic interfacial potential ( 2 . 4 ) . By inspection of ( 2 . 4 ) , ( 4 .
14 ) thus becomes Pzz ( 0 , x ) = [ 2u / ( 1 – 20 ) ] ( W / d ) ( B . 1 ) It has only been
possible to solve the elastic problem with this extra boundary condition , for the
unrealistic parabolic interfacial potential ( 2 . 4 ) . By inspection of ( 2 . 4 ) , ( 4 .
Page 240
At a field H . 1 it becomes energetically favorable to produce flux lines . In
complete analogy to Eq . ( 10 ) , H . 1 can be expressed in terms of the free
energy per length of a flux line E . ( for H = 0 ) and the reduction in magnetic field
energy – P ...
At a field H . 1 it becomes energetically favorable to produce flux lines . In
complete analogy to Eq . ( 10 ) , H . 1 can be expressed in terms of the free
energy per length of a flux line E . ( for H = 0 ) and the reduction in magnetic field
energy – P ...
Page 255
For higher To materials , as the coherence length of the superconducting
electrons becomes smaller , the tunneling results become more dependent on
the surface properties . Thus , the tunneling results for the A - 15 compounds are
...
For higher To materials , as the coherence length of the superconducting
electrons becomes smaller , the tunneling results become more dependent on
the surface properties . Thus , the tunneling results for the A - 15 compounds are
...
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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