Treatise on Materials Science and TechnologyHerbert Herman |
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Page 53
... layer but are inadequate for thicker ones , because they do not allow for the proper elastic relaxation in substrate and film . The model of Ball ( 1970 ) , described in Section V , C , is an improve- ment on the former , since it makes ...
... layer but are inadequate for thicker ones , because they do not allow for the proper elastic relaxation in substrate and film . The model of Ball ( 1970 ) , described in Section V , C , is an improve- ment on the former , since it makes ...
Page 148
... layer crystals of total thickness Dlay . For a good monochromator the △ t has then to be larger than △ t / instead of larger than △ t , which was required for ideal mosaic or layer crystal . This is fulfilled for a lot of crystals ...
... layer crystals of total thickness Dlay . For a good monochromator the △ t has then to be larger than △ t / instead of larger than △ t , which was required for ideal mosaic or layer crystal . This is fulfilled for a lot of crystals ...
Page 192
... layer the [ 001 ] -direction a ky M Fig . 25. View along the [ 001 ] axis in the perovskite structure . The linked ... layers ; critical point R for the case of 180 ° antiphase layers . has exactly the same rotation angle & in the same ...
... layer the [ 001 ] -direction a ky M Fig . 25. View along the [ 001 ] axis in the perovskite structure . The linked ... layers ; critical point R for the case of 180 ° antiphase layers . has exactly the same rotation angle & in the same ...
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