Treatise on Materials Science and TechnologyHerbert Herman |
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Page 36
... considered in greater detail in Section VIII . 5. FILM THICKNESS The foregoing analysis is based on the assumption , among others , that the substrate is rigid and the strain gradient perpendicular to the film plane vanishes . Although ...
... considered in greater detail in Section VIII . 5. FILM THICKNESS The foregoing analysis is based on the assumption , among others , that the substrate is rigid and the strain gradient perpendicular to the film plane vanishes . Although ...
Page 75
... considered in this section . In these the interfaces were initially sharp with misfit dislocations located in them . Inter- diffusion took place on annealing , which results in a redistribution of the misfit dislocations over the ...
... considered in this section . In these the interfaces were initially sharp with misfit dislocations located in them . Inter- diffusion took place on annealing , which results in a redistribution of the misfit dislocations over the ...
Page 334
... considered to be ferromagnetically coupled ; in other words , their magnetic moments are added . The a - site and the c - site cation sublattices are in most cases considered to be ferromagnetically coupled . The d - site cation ...
... considered to be ferromagnetically coupled ; in other words , their magnetic moments are added . The a - site and the c - site cation sublattices are in most cases considered to be ferromagnetically coupled . The d - site cation ...
Contents
Epitaxial Interfaces | 3 |
Thin Films | 15 |
Semiinfinite Overgrowths | 37 |
Copyright | |
11 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 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 tetrahedral thermal thickness transition metal values vector X-ray YGaG