Treatise on Materials Science and TechnologyHerbert Herman |
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Results 1-3 of 44
Page 94
... yields U = CX μ + р where - 200 1 = ( 1-0a , b ) / Ma , b b ― - 1 ( B.13 ) ( B.14 ) By substitution of ( B.9 ) into ... yield , when combined with ( B.10 ) , the following equations for S1 and R : -1 1 Sn + v ̄1v_d [ m + vd ̄1 ( μ71 + ...
... yields U = CX μ + р where - 200 1 = ( 1-0a , b ) / Ma , b b ― - 1 ( B.13 ) ( B.14 ) By substitution of ( B.9 ) into ... yield , when combined with ( B.10 ) , the following equations for S1 and R : -1 1 Sn + v ̄1v_d [ m + vd ̄1 ( μ71 + ...
Page 254
... yield a direct value of the renormalized electron density of states at the Fermi level . However , in materials with high critical fields H. 2 , it is not possible to suppress the superconducting transition . In compounds such as the A ...
... yield a direct value of the renormalized electron density of states at the Fermi level . However , in materials with high critical fields H. 2 , it is not possible to suppress the superconducting transition . In compounds such as the A ...
Page 268
... yields a value of the order of 10 g / mm2 . Experiments on type I and type II superconductors show , however , a drop in yield stress of the order of a few percent at the transition from normal to superconducting state ( Kajima and ...
... yields a value of the order of 10 g / mm2 . Experiments on type I and type II superconductors show , however , a drop in yield stress of the order of a few percent at the transition from normal to superconducting state ( Kajima and ...
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