Treatise on Materials Science and TechnologyHerbert Herman |
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Page 236
... field cannot penetrate into a type I superconductor . The magnetic field cannot , however , go to zero dis- continuously at the surface of the superconductor since this would require infinite shielding - current densities at the surface ...
... field cannot penetrate into a type I superconductor . The magnetic field cannot , however , go to zero dis- continuously at the surface of the superconductor since this would require infinite shielding - current densities at the surface ...
Page 237
Herbert Herman. field H1 , the field will penetrate into the normal metal but not into the super- conductor . To get the difference of the free energies for H , 0 , we therefore have to add the field expulsion energy density H2 / 8π ...
Herbert Herman. field H1 , the field will penetrate into the normal metal but not into the super- conductor . To get the difference of the free energies for H , 0 , we therefore have to add the field expulsion energy density H2 / 8π ...
Page 302
... field effects on cations , especially the transition metal ions , has been studied extensively . There are many significant achievements in this field and numerous books and treatises on this subject ( Orgel , 1960 ; Griffith , 1961 ...
... field effects on cations , especially the transition metal ions , has been studied extensively . There are many significant achievements in this field and numerous books and treatises on this subject ( Orgel , 1960 ; Griffith , 1961 ...
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