Treatise on Materials Science and TechnologyHerbert Herman |
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Page 143
... sample and lens area , maximum length , etc. The consideration above holds for unbent single crystals as samples . Improvement can be obtained in high resolution work with powders placing them along the focal circle and could in ...
... sample and lens area , maximum length , etc. The consideration above holds for unbent single crystals as samples . Improvement can be obtained in high resolution work with powders placing them along the focal circle and could in ...
Page 174
... samples is well separated from the background values ( after 300 ° K annealing ) , which are mainly thermal diffuse ... sample . The small change between these two curves is explained by Ehrhart by the competing processes of partial ...
... samples is well separated from the background values ( after 300 ° K annealing ) , which are mainly thermal diffuse ... sample . The small change between these two curves is explained by Ehrhart by the competing processes of partial ...
Page 353
... samples , the sample of 99 % density had a maximum AH of 15 Oe , and the sample of 79 % had a maximum AH of 420 Oe ( Patton , 1970 ) . Although there are no known data reported , this degenerate mode linewidth can be used to study the ...
... samples , the sample of 99 % density had a maximum AH of 15 Oe , and the sample of 79 % had a maximum AH of 420 Oe ( Patton , 1970 ) . Although there are no known data reported , this degenerate mode linewidth can be used to study the ...
Contents
Epitaxial Interfaces | 3 |
Thin Films | 15 |
Semiinfinite Overgrowths | 37 |
Copyright | |
13 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 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