Treatise on Materials Science and Technology, Volume 2 |
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Page 108
A rough guide is that the simplicity of scattering functions gives averaged values
in a proper form , whereas electron ... They give very specific scattering patterns
near reciprocal lattice points depending on the relative orientation of the ...
A rough guide is that the simplicity of scattering functions gives averaged values
in a proper form , whereas electron ... They give very specific scattering patterns
near reciprocal lattice points depending on the relative orientation of the ...
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 168
H ( K ) gives an important contribution in the region between Bragg reflections , if
defects have large distortions like interstitials , as shown by Eisenriegler ( 1972 )
recently . The crucial term in Eq . ( 47 ) is the linear displacement term iks ) ( K ) .
H ( K ) gives an important contribution in the region between Bragg reflections , if
defects have large distortions like interstitials , as shown by Eisenriegler ( 1972 )
recently . The crucial term in Eq . ( 47 ) is the linear displacement term iks ) ( K ) .
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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