Treatise on Materials Science and TechnologyHerbert Herman |
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Page 235
... superconductor can be found from thermo- dynamic arguments . The field energy H.2 / 8ะป at the critical field must be the difference in free energy between the superconducting and normal states PROPERTIES OF SUPERCONDUCTING MATERIALS 235.
... superconductor can be found from thermo- dynamic arguments . The field energy H.2 / 8ะป at the critical field must be the difference in free energy between the superconducting and normal states PROPERTIES OF SUPERCONDUCTING MATERIALS 235.
Page 236
... superconducting and normal areas cannot be discontinuous . Changes in the density n , of Cooper pairs cannot occur ... superconducting area . Let AGso be the difference between the specific free energy of a metal in the superconducting ...
... superconducting and normal areas cannot be discontinuous . Changes in the density n , of Cooper pairs cannot occur ... superconducting area . Let AGso be the difference between the specific free energy of a metal in the superconducting ...
Page 255
... SUPERCONDUCTING PROPERTIES c The study of physical properties in the superconducting state is a most important means of verifying the predictions of any theory of transition metals superconductivity . The most basic are thermodynamic ...
... SUPERCONDUCTING PROPERTIES c The study of physical properties in the superconducting state is a most important means of verifying the predictions of any theory of transition metals superconductivity . The most basic are thermodynamic ...
Contents
Epitaxial Interfaces | 3 |
Thin Films | 15 |
Semiinfinite Overgrowths | 37 |
Copyright | |
11 other sections not shown
Common terms and phrases
angle anisotropy Appl approximation assumed atoms average axis c-sites calculated cations coherent 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 interaction interface ions lattice length Lett 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 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