Treatise on Materials Science and TechnologyHerbert Herman |
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Page 115
... Powders , for which the refractive index for neutrons and hence the averaged coherent scattering length has to be ... powder . With this method , the coherent scattering lengths of nearly all elements can be deter- mined with an ...
... Powders , for which the refractive index for neutrons and hence the averaged coherent scattering length has to be ... powder . With this method , the coherent scattering lengths of nearly all elements can be deter- mined with an ...
Page 149
... powder diffraction and therefore often are useless in single crystal diffraction for reasons already shown in Section III , A. ii . The author has the impression that X - ray designs are in some cases far from an optimized stage if ...
... powder diffraction and therefore often are useless in single crystal diffraction for reasons already shown in Section III , A. ii . The author has the impression that X - ray designs are in some cases far from an optimized stage if ...
Page 150
... individual strips have been constructed by Jacobet and Allemagne ( Grenoble ) . A multi- detector system with 200 elements is in operation for powder diffractometry at the Siloe reactor in Grenoble , and a crossed strip 150 W. SCHMATZ.
... individual strips have been constructed by Jacobet and Allemagne ( Grenoble ) . A multi- detector system with 200 elements is in operation for powder diffractometry at the Siloe reactor in Grenoble , and a crossed strip 150 W. SCHMATZ.
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