## Treatise on Materials Science and Technology, Volume 2 |

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Page 235

76kB T . = 40 ( 4 ) where A , is one - half the

zero of temperature . ... lack of electrical resistance in the

we first note that the Cooper pairs in a

76kB T . = 40 ( 4 ) where A , is one - half the

**superconducting**gap at the absolutezero 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

absolute zero the ... B . Type II Superconductivity ( 0 ) Because of the Meissner

effect , an external field cannot penetrate into a type I

magnetic ...

difference in free energy between the

**superconducting**and normal states . Atabsolute zero the ... B . Type II Superconductivity ( 0 ) Because of the Meissner

effect , an external field cannot penetrate into a type I

**superconductor**. Themagnetic ...

Page 255

The tunneling results that depend both on the electron - phonon matrix elements

and the phonon density of states in the transition metal

analyzed with McMillan ' s formulation . A value of 1 = 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**wereanalyzed with McMillan ' s formulation . A value of 1 = 0 . 69 for Ta was found in ...

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angle anisotropy approximation assumed atoms average axis c-sites calculated cations coherent compounds concentration condition considerations constant contribution corresponding crystal curve defect density dependence determined diffusion direction discussed dislocations displacement effect elastic elastic scattering electron energy equation et al exist experimental experiments factor field flux lines follows force function garnet given gives important increasing Inelastic Scattering interaction interface ions lattice length limit magnetic materials measured Merwe metal method misfit mode neutron normal obtained parameter phase phonon Phys plane position potential present properties range rare earth reference region relation resolution resonance 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 X-ray