Treatise on Materials Science and Technology, Volume 2 |
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Results 1-3 of 52
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 125
In many cases , sufficient experimental data are available to take ph . ; into
account in defect scattering . A comment is necessary concerning integrated one
- phonon scattering cross sections . For X - rays , the contribution of one branch
for a ...
In many cases , sufficient experimental data are available to take ph . ; into
account in defect scattering . A comment is necessary concerning integrated one
- phonon scattering cross sections . For X - rays , the contribution of one branch
for a ...
Page 172
The wavelength dependence of the defect induced change in total cross section
and the angular dependence of the scattering cross section have been used as
an indication for defect clusters ( BeO ) , for amorphous zones ( SiO2 ) , and for ...
The wavelength dependence of the defect induced change in total cross section
and the angular dependence of the scattering cross section have been used as
an indication for defect clusters ( BeO ) , for amorphous zones ( SiO2 ) , and for ...
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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