Treatise on Materials Science and TechnologyHerbert Herman |
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Results 1-3 of 35
Page 92
... becomes x Pzz ( 0 , x ) = [ 2μ / ( 1-20 ) ] ( W / d ) ( B.1 ) It has only been possible to solve the elastic problem with this extra boundary condition , for the unrealistic parabolic interfacial potential ( 2.4 ) . By inspection of ...
... becomes x Pzz ( 0 , x ) = [ 2μ / ( 1-20 ) ] ( W / d ) ( B.1 ) It has only been possible to solve the elastic problem with this extra boundary condition , for the unrealistic parabolic interfacial potential ( 2.4 ) . By inspection of ...
Page 240
... becomes energetically favorable to produce flux lines . In complete analogy to Eq . ( 10 ) , He1 can be expressed in terms of the free energy per length of a flux line & o ( for H2 = 0 ) and the reduction in magnetic field energy - Ha ...
... becomes energetically favorable to produce flux lines . In complete analogy to Eq . ( 10 ) , He1 can be expressed in terms of the free energy per length of a flux line & o ( for H2 = 0 ) and the reduction in magnetic field energy - Ha ...
Page 255
... becomes smaller , the tunneling results become more dependent on the surface properties . Thus , the tunneling results for the A - 15 compounds are unreliable indicators of bulk properties . Hopfield ( 1972 ) has recently argued that a ...
... becomes smaller , the tunneling results become more dependent on the surface properties . Thus , the tunneling results for the A - 15 compounds are unreliable indicators of bulk properties . Hopfield ( 1972 ) has recently argued that a ...
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