Treatise on Materials Science and Technology, Volume 2 |
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Page 237
Herbert Herman. field Ha , the field will penetrate into the normal metal but not
into the superconductor . To get the difference of the free energies for H , + 0 , we
therefore have to add the field expulsion energy density H , ? / 87 . Thus we get
for ...
Herbert Herman. field Ha , the field will penetrate into the normal metal but not
into the superconductor . To get the difference of the free energies for H , + 0 , we
therefore have to add the field expulsion energy density H , ? / 87 . Thus we get
for ...
Page 254
ELECTRON PROPERTIES Inasmuch as a net attractive interaction between
electrons due to the electron - phonon interaction is expected for quasi - particle
energy & SOD , information about the electronic density of states near the Fermi ...
ELECTRON PROPERTIES Inasmuch as a net attractive interaction between
electrons due to the electron - phonon interaction is expected for quasi - particle
energy & SOD , information about the electronic density of states near the Fermi ...
Page 262
with the critical current density J . ( r ) . The physical facts underlying Eqs . ( 24 )
and ( 25 ) gave rise to a great many discussions and misunderstandings , before
the situation was clarified by Josephson ( 1965 , 1966 ) and Evetts et al . ( 1968 )
.
with the critical current density J . ( r ) . The physical facts underlying Eqs . ( 24 )
and ( 25 ) gave rise to a great many discussions and misunderstandings , before
the situation was clarified by Josephson ( 1965 , 1966 ) and Evetts et al . ( 1968 )
.
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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