Treatise on Materials Science and TechnologyHerbert Herman |
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Page 236
... field H. ( 0 ) is given by Н ̧ ( 0 ) 2 / 8π = 1 / 2N ( 0 ) A2 The critical field falls off with increasing temperature approximately as H ( T ) / H ̧ ( 0 ) = 1 ... field H2 , the field will penetrate into 236 F. Y. FRADIN AND P. NEUMANN.
... field H. ( 0 ) is given by Н ̧ ( 0 ) 2 / 8π = 1 / 2N ( 0 ) A2 The critical field falls off with increasing temperature approximately as H ( T ) / H ̧ ( 0 ) = 1 ... field H2 , the field will penetrate into 236 F. Y. FRADIN AND P. NEUMANN.
Page 237
Herbert Herman. a a field H2 , the field will penetrate into the normal metal but not into the super- conductor . To get the difference of the free energies for H1 0 , we therefore have to add the field expulsion energy density H2 / 87 ...
Herbert Herman. a a field H2 , the field will penetrate into the normal metal but not into the super- conductor . To get the difference of the free energies for H1 0 , we therefore have to add the field expulsion energy density H2 / 87 ...
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 | |
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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 R₁ 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 thermal thickness transition metal values vector X-ray YGaG νμ ΦΩ