Treatise on Materials Science and TechnologyHerbert Herman |
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Page 39
... planes through these centers . In principle therefore these planes are also the interfacial planes of the elastic continua . Mathematically the plane z = 0 is thus assumed to be one of these , the specific one depending on which crystal ...
... planes through these centers . In principle therefore these planes are also the interfacial planes of the elastic continua . Mathematically the plane z = 0 is thus assumed to be one of these , the specific one depending on which crystal ...
Page 76
... plane . If this crystal is straightened as in Fig . 29 ( c ) , a constant gradient of strain in the direction of z is set up resulting in a compression above and an extension below the dotted neutral plane AA ' . A close similarity with ...
... plane . If this crystal is straightened as in Fig . 29 ( c ) , a constant gradient of strain in the direction of z is set up resulting in a compression above and an extension below the dotted neutral plane AA ' . A close similarity with ...
Page 137
... plane , i.e. , the plane containing ko and k1 , is often a symmetry plane of the crystal investigated . In such cases Ŝ ( k , ) is equal to Ŝ ( −κ , ) and therefore Ŝ ( ) is an extremum with respect to κ ,. This means Ŝ changes in ...
... plane , i.e. , the plane containing ko and k1 , is often a symmetry plane of the crystal investigated . In such cases Ŝ ( k , ) is equal to Ŝ ( −κ , ) and therefore Ŝ ( ) is an extremum with respect to κ ,. This means Ŝ changes in ...
Contents
Epitaxial Interfaces | 3 |
Thin Films | 15 |
Semiinfinite Overgrowths | 37 |
Copyright | |
11 other sections not shown
Common terms and phrases
angle anisotropy Appl approximation assumed atoms average axis c-sites calculated cations coherent concentration condition considerations constant contribution corresponding crystal curve defect density dependence determined diffusion direction discussed dislocations displacement effect elastic elastic scattering electron energy equation et al exist experimental experiments factor field flux lines follows force function garnet given gives important increasing interaction interface ions lattice length Lett limit magnetic materials measured Merwe metal method misfit mode neutron normal obtained parameter phase phonon Phys plane position potential present properties range rare earth reference region relation 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 X-ray