Treatise on Materials Science and Technology, Volume 2 |
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Page 197
In the foc lattice the two different sites are isotropic but the different sites give
slightly different structure factors for the fundamental Bragg reflections . For the a
phase of H and D in Pd Nelin ( 1971 ) has determined the structure factor in a
very ...
In the foc lattice the two different sites are isotropic but the different sites give
slightly different structure factors for the fundamental Bragg reflections . For the a
phase of H and D in Pd Nelin ( 1971 ) has determined the structure factor in a
very ...
Page 355
The magnetic anisotropy in the rare earth garnets can be understood by the g -
factor values . The agreement between experiments and theoretical calculations
is very good , as shown in Table XVIII . As discussed in Section III , E and shown
...
The magnetic anisotropy in the rare earth garnets can be understood by the g -
factor values . The agreement between experiments and theoretical calculations
is very good , as shown in Table XVIII . As discussed in Section III , E and shown
...
Page 371
The ratio Kolkó is called the crystal complexity factor G ( Oliver and Slack , 1966 )
. The values of Ko , Ko ' , and G , for several garnets are listed in Table XXIX (
Slack and Oliver , 1971 ) . The crystal complexity factor G varies from 0 . 080 to 0 .
The ratio Kolkó is called the crystal complexity factor G ( Oliver and Slack , 1966 )
. The values of Ko , Ko ' , and G , for several garnets are listed in Table XXIX (
Slack and Oliver , 1971 ) . The crystal complexity factor G varies from 0 . 080 to 0 .
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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