Treatise on Materials Science and TechnologyHerbert Herman |
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Page 13
... additional area A is covered such as at 1 , is negative , as compared to an addition at 2 , where there is no change in f . 2 B AB SUBSTRATE Fig . 6. Diagram representing a monolayer B on a substrate A. The dotted rectangles indicate ...
... additional area A is covered such as at 1 , is negative , as compared to an addition at 2 , where there is no change in f . 2 B AB SUBSTRATE Fig . 6. Diagram representing a monolayer B on a substrate A. The dotted rectangles indicate ...
Page 67
... additional ones other than that an interfacial potential exists . The application of ( i ) introduces additional approximations , but has the advantage of allowing one to use either the simple or the refined model and is hopefully ...
... additional ones other than that an interfacial potential exists . The application of ( i ) introduces additional approximations , but has the advantage of allowing one to use either the simple or the refined model and is hopefully ...
Page 173
... additional expansion in transition from infinite to finite medium is homogeneous and has negligible influence on the ... addition with sufficient data at different tempera- tures and concentrations the double force tensor , i.e. , more ...
... additional expansion in transition from infinite to finite medium is homogeneous and has negligible influence on the ... addition with sufficient data at different tempera- tures and concentrations the double force tensor , i.e. , more ...
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