Treatise on Materials Science and Technology, Volume 2 |
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Page 235
76kB T . = 40 ( 4 ) where A , is one - half the superconducting gap at the absolute
zero of temperature . ... lack of electrical resistance in the superconducting state ,
we first note that the Cooper pairs in a superconductor have zero total spin and ...
76kB T . = 40 ( 4 ) where A , is one - half the superconducting gap at the absolute
zero of temperature . ... lack of electrical resistance in the superconducting state ,
we first note that the Cooper pairs in a superconductor have zero total spin and ...
Page 236
difference in free energy between the superconducting and normal states . At
absolute zero the ... B . Type II Superconductivity Because of the Meissner effect ,
an external field cannot penetrate into a type I superconductor . The magnetic
field ...
difference in free energy between the superconducting and normal states . At
absolute zero the ... B . Type II Superconductivity Because of the Meissner effect ,
an external field cannot penetrate into a type I superconductor . The magnetic
field ...
Page 255
The tunneling results that depend both on the electron - phonon matrix elements
and the phonon density of states in the transition metal superconductor were
analyzed with McMillan ' s formulation . A value of 2 = 0 . 69 for Ta was found in ...
The tunneling results that depend both on the electron - phonon matrix elements
and the phonon density of states in the transition metal superconductor were
analyzed with McMillan ' s formulation . A value of 2 = 0 . 69 for Ta was found in ...
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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