Treatise on Materials Science and TechnologyHerbert Herman |
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Page 5
... present it is adequate to regard the interfacial atomic symmetry as being quadratic with atomic spacings a and b . The model disregards the superstructures , which are observed by LEED and are not completely understood . It is suggested ...
... present it is adequate to regard the interfacial atomic symmetry as being quadratic with atomic spacings a and b . The model disregards the superstructures , which are observed by LEED and are not completely understood . It is suggested ...
Page 11
... present calculations are measured in units of Q , changes in & , cannot be ignored completely . a The tangential forces discussed above introduce curvatures into the crystal surfaces at the interface , whereby opposite points are ...
... present calculations are measured in units of Q , changes in & , cannot be ignored completely . a The tangential forces discussed above introduce curvatures into the crystal surfaces at the interface , whereby opposite points are ...
Page 89
... present approach , and those of Vincent and others . It is to be noted that the model used to demonstrate the saw - tooth behavior is a severely oversimplified representation of the physical system . The model is , among others , one ...
... present approach , and those of Vincent and others . It is to be noted that the model used to demonstrate the saw - tooth behavior is a severely oversimplified representation of the physical system . The model is , among others , one ...
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