Treatise on Materials Science and Technology, Volume 2 |
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Page 53
mately to a two - fold atomic layer , while those of the infinite case are highly
accurate representations for an overgrowth of finite thickness provided the
thickness exceeds half the spacing between misfit dislocations . Evidently a wide
and ...
mately to a two - fold atomic layer , while those of the infinite case are highly
accurate representations for an overgrowth of finite thickness provided the
thickness exceeds half the spacing between misfit dislocations . Evidently a wide
and ...
Page 148
From experimental data we take a quality factor Q ( < 1 ) defined as the ratio of
actual integrated reflectivity to the ideal mosaic integral reflectivity in case of
mosaic crystals and Dlay , min / Dlay in case of layer crystals of total thickness
Diay .
From experimental data we take a quality factor Q ( < 1 ) defined as the ratio of
actual integrated reflectivity to the ideal mosaic integral reflectivity in case of
mosaic crystals and Dlay , min / Dlay in case of layer crystals of total thickness
Diay .
Page 192
If in the next layer the [ 001 ] - direction 2 0 0 - - - - 0 - - NO Fig . 25 . ... Critical
point M for the case of equal $ in successive layers ; critical point R for the case of
180° antiphase layers . has exactly the same rotation angle o in the same 192 W
...
If in the next layer the [ 001 ] - direction 2 0 0 - - - - 0 - - NO Fig . 25 . ... Critical
point M for the case of equal $ in successive layers ; critical point R for the case of
180° antiphase layers . has exactly the same rotation angle o in the same 192 W
...
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Contents
Epitaxial Interfaces | 3 |
Thin Films | 15 |
Semiinfinite Overgrowths | 52 |
Copyright | |
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Common terms and phrases
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