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 | |
13 other sections not shown
Common terms and phrases
a-site alloy Amer anisotropy Appl approximation atoms average axis B₁ Bragg Bragg reflections c-sites calculated cations coefficients coherent compounds concentration configuration constant Cooper pairs curve Debye-Waller factor defect density dependence discussed displacement elastic electron energy epitaxial equation experimental factor ferrimagnetic field film flux lines function garnet garnet structure GdIG Geller IAEA impurity Inelastic Scattering interaction interface iron garnets k₁ lattice constant lattice parameter Lett magnetic magnetocrystalline anisotropy measured Merwe method misfit misfit dislocations mode neutron scattering normal obtained overgrowth phase phonon Phys plane potential Proc properties R₁ rare earth rare earth ions reciprocal lattice resolution sample scattering cross section shown in Fig single crystal small angle solid strain stress sublattice substrate superconducting surface symmetry Table temperature thermal thickness transition metal values vector X-ray YGaG νμ ΦΩ