Treatise on Materials Science and Technology, Volume 2 |
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Page 106
For an ideal mosaic crystal , it is sufficient to determine integrated reflectivities of
Bragg reflections in order to deduce the structure . Crystal imperfections normally
have little influence on the integrated reflectivities as long as a sufficiently large ...
For an ideal mosaic crystal , it is sufficient to determine integrated reflectivities of
Bragg reflections in order to deduce the structure . Crystal imperfections normally
have little influence on the integrated reflectivities as long as a sufficiently large ...
Page 165
Experimental evidence cited to support this erroneous view are peaks in the
diffuse scattering found by Austermann and Miller ( 1965 ) at the original position
of Bragg reflections in heavily neutron irradiated BeO powder . Since in such ...
Experimental evidence cited to support this erroneous view are peaks in the
diffuse scattering found by Austermann and Miller ( 1965 ) at the original position
of Bragg reflections in heavily neutron irradiated BeO powder . Since in such ...
Page 171
In this case the scattering is asymmetric with respect to the Bragg reflection
because the iksp ( K ) term changes sign for q crossing the Bragg reflection . The
scattering patterns in the vicinity of Bragg reflections as they can be determined
from ...
In this case the scattering is asymmetric with respect to the Bragg reflection
because the iksp ( K ) term changes sign for q crossing the Bragg reflection . The
scattering patterns in the vicinity of Bragg reflections as they can be determined
from ...
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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