Treatise on Materials Science and TechnologyHerbert Herman |
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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
angle anisotropy Appl approximation assumed atoms average axis c-sites calculated cations coherent concentration condition considerations constant contribution corresponding crystal curve defect density dependence determined diffusion direction discussed dislocations displacement effect elastic elastic scattering electron energy equation et al exist experimental experiments factor field flux lines follows force function garnet given gives important increasing interaction interface ions lattice length Lett limit magnetic materials measured Merwe metal method misfit mode neutron normal obtained parameter phase phonon Phys plane position potential present properties range rare earth reference region relation resolution respectively sample scattering cross section shown shows single solid solution space strain stress structure substrate superconducting surface Table temperature tetrahedral theory thermal thickness transition unit values vector X-ray