Treatise on Materials Science and TechnologyHerbert Herman |
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Results 1-3 of 37
Page 120
... scattering cross section consisting of two parts : the elastic scattering cross section with 8 ( w ) and the inelastic scattering cross section . For the elastic scattering cross section , we obtain do VO ikr VO G ikr ( da ) = Σ be , c ...
... scattering cross section consisting of two parts : the elastic scattering cross section with 8 ( w ) and the inelastic scattering cross section . For the elastic scattering cross section , we obtain do VO ikr VO G ikr ( da ) = Σ be , c ...
Page 140
... scattering is dominant , it may be sufficient to monochromatize only the incident or scattered beam . Inelastic ... elastic scattering is proportional to Ak ,. Thus the elastic scattering can be made dominant with increasing resolution ...
... scattering is dominant , it may be sufficient to monochromatize only the incident or scattered beam . Inelastic ... elastic scattering is proportional to Ak ,. Thus the elastic scattering can be made dominant with increasing resolution ...
Page 202
... scattering also . This can be of considerable value for the quasielastic band mode and localized mode scattering , as seen previously in discussing metal alloy scattering ; however because of the smaller cross section it requires higher ...
... scattering also . This can be of considerable value for the quasielastic band mode and localized mode scattering , as seen previously in discussing metal alloy scattering ; however because of the smaller cross section it requires higher ...
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