Treatise on Materials Science and Technology, Volume 2 |
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Page 4
... when the misfit and thickness are small enough , is one in which the
overgrowth is coherent , i . e . , the misfit is entirely accommodated by
homogeneous lateral strain in the overgrowth ; ( iii ) beyond certain values of
misfit and / or thickness ...
... when the misfit and thickness are small enough , is one in which the
overgrowth is coherent , i . e . , the misfit is entirely accommodated by
homogeneous lateral strain in the overgrowth ; ( iii ) beyond certain values of
misfit and / or thickness ...
Page 53
Evidently a wide and important range of overgrowth thicknesses are thereby
excluded . An exact ( van der Merwe , 1963b ) though complicated solution of the
problem concerning overgrowths of intermediate thickness is presented using the
...
Evidently a wide and important range of overgrowth thicknesses are thereby
excluded . An exact ( van der Merwe , 1963b ) though complicated solution of the
problem concerning overgrowths of intermediate thickness is presented using the
...
Page 332
The above equation is for the simplest case where the moduli of elasticity and the
thicknesses of the film and the ... a film thickness greater than 3 um , and the
GDIG films on GdGaG cracked at a film thickness greater than 5 um ( Stein and ...
The above equation is for the simplest case where the moduli of elasticity and the
thicknesses of the film and the ... a film thickness greater than 3 um , and the
GDIG films on GdGaG cracked at a film thickness greater than 5 um ( Stein and ...
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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