Treatise on Materials Science and TechnologyHerbert Herman |
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Page 236
... depth 2 ( London and London , 1935a , b ) , which is of the order of a few 100 Å for all superconductors . For flat macroscopic surfaces , the London theory gives ( assuming Cooper pairs as current carriers ) : 22 λ2 = 2mc2 / 4πn , ( 2e ) ...
... depth 2 ( London and London , 1935a , b ) , which is of the order of a few 100 Å for all superconductors . For flat macroscopic surfaces , the London theory gives ( assuming Cooper pairs as current carriers ) : 22 λ2 = 2mc2 / 4πn , ( 2e ) ...
Page 259
... depth 2 . Under the magnetic pressure of the applied field , the flux lines form a triangular lattice that was predicted theoretically ( Kleiner et al . , 1964 ; Matricon , 1964 ) ( see Fig . 5 ) and verified experimentally by such ...
... depth 2 . Under the magnetic pressure of the applied field , the flux lines form a triangular lattice that was predicted theoretically ( Kleiner et al . , 1964 ; Matricon , 1964 ) ( see Fig . 5 ) and verified experimentally by such ...
Page 321
... depth of melt in the crucible ; the rate of pulling ; and the latent heat of fusion . Iron garnets , being incongruently melting compounds , cannot be grown by the Czochralski method . On the other hand , aluminum and gallium garnets ...
... depth of melt in the crucible ; the rate of pulling ; and the latent heat of fusion . Iron garnets , being incongruently melting compounds , cannot be grown by the Czochralski method . On the other hand , aluminum and gallium garnets ...
Contents
Epitaxial Interfaces | 3 |
Thin Films | 15 |
Semiinfinite Overgrowths | 37 |
Copyright | |
11 other sections not shown
Common terms and phrases
a-site alloy Amer anisotropy Appl approximation atoms average axis B₁ Bragg Bragg reflections c-sites calculated cations coefficients coherent compounds concentration configuration constant Cooper pairs curve Debye-Waller factor defect density dependence discussed displacement elastic electron energy epitaxial equation experimental factor ferrimagnetic field film flux lines function garnet garnet structure GdIG Geller IAEA impurity Inelastic Scattering interaction interface iron garnets k₁ lattice constant lattice parameter Lett magnetic magnetocrystalline anisotropy measured Merwe method misfit misfit dislocations mode neutron scattering normal obtained overgrowth phase phonon Phys plane potential Proc properties rare earth rare earth ions reciprocal lattice resolution sample scattering cross section shown in Fig single crystal small angle solid strain stress sublattice substrate superconducting surface symmetry Table temperature tetrahedral thermal thickness transition metal values vector X-ray YGaG