Treatise on Materials Science and Technology, Volume 2 |
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Page 120
Substitution of Eq . ( 52 ) into Eq . ( 48 ) gives a scattering cross section consisting
of two parts : the elastic scattering cross section with S ( w ) and the inelastic
scattering cross section . For the elastic scattering cross section , we obtain 0
Simiv ...
Substitution of Eq . ( 52 ) into Eq . ( 48 ) gives a scattering cross section consisting
of two parts : the elastic scattering cross section with S ( w ) and the inelastic
scattering cross section . For the elastic scattering cross section , we obtain 0
Simiv ...
Page 140
If elastic scattering is dominant , it may be sufficient to monochromatize only the
incident or scattered beam . Inelastic scattering contributions can be reduced by
monochromatizing both beams , whereby similar shape of fo and fı with respect to
...
If elastic scattering is dominant , it may be sufficient to monochromatize only the
incident or scattered beam . Inelastic scattering contributions can be reduced by
monochromatizing both beams , whereby similar shape of fo and fı with respect to
...
Page 202
A first attempt in this direction has been made by a study of the integral coherent
quasielastic scattering cross section ( Conrad and Bauer , 1972 ) . The results
can be handled within the theory of elastic scattering for binary alloys after ...
A first attempt in this direction has been made by a study of the integral coherent
quasielastic scattering cross section ( Conrad and Bauer , 1972 ) . The results
can be handled within the theory of elastic scattering for binary alloys after ...
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Contents
Epitaxial Interfaces | 3 |
Thin Films | 15 |
Semiinfinite Overgrowths | 52 |
Copyright | |
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angle anisotropy approximation assumed atoms average axis c-site calculated cations coherent compounds concentration condition considerations constants contribution corresponding crystal curve decreases defect density dependence determined diffusion direction discussed dislocations displacement effect elastic elastic scattering electron energy equation et al experimental experiments factor field flux flux lines follows force function garnets given gives important impurity increases interaction interface ions lattice limit magnetic materials measured Merwe metal method misfit mode neutron normal observed obtained optical parameter phase phonon Phys plane position potential present processes properties range reference region 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 wave X-ray