Treatise on Materials Science and TechnologyHerbert Herman |
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Page 221
... copper precipitate is contracted . The asymmetry caused by the sign change of Adiv diminishes the intensity for qantiparallel to Thkl dramatically in this special case . The total resulting scattering pattern around 200 is shown ...
... copper precipitate is contracted . The asymmetry caused by the sign change of Adiv diminishes the intensity for qantiparallel to Thkl dramatically in this special case . The total resulting scattering pattern around 200 is shown ...
Page 231
... copper . Just below its transition temperature , the alloy's resistance has essentially disappeared . The copper now is an insulator by comparison . † Work performed under the auspices of the U.S. Atomic Energy Commission . ‡ Present ...
... copper . Just below its transition temperature , the alloy's resistance has essentially disappeared . The copper now is an insulator by comparison . † Work performed under the auspices of the U.S. Atomic Energy Commission . ‡ Present ...
Page 232
... Copper 10-7 10-8 10-9 3 10 30 100 300 Temperature ( ° K ) Fig . 1. Electrical resistivity vs. temperature for high - purity copper and a Nb - Ti alloy . Resistivity of the alloy vanishes below 9 ° K , its superconducting critical ...
... Copper 10-7 10-8 10-9 3 10 30 100 300 Temperature ( ° K ) Fig . 1. Electrical resistivity vs. temperature for high - purity copper and a Nb - Ti alloy . Resistivity of the alloy vanishes below 9 ° K , its superconducting critical ...
Contents
Epitaxial Interfaces | 3 |
Thin Films | 15 |
Semiinfinite Overgrowths | 37 |
Copyright | |
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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