Treatise on Materials Science and TechnologyHerbert Herman |
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Page 7
... term and having adjusted the coefficients such that the potential is zero at the lowest point has been introduced by Frenkel and Kontorowa ( 1938 ) in a model which has since been applied to epitaxial monolayers ( Frank and van der ...
... term and having adjusted the coefficients such that the potential is zero at the lowest point has been introduced by Frenkel and Kontorowa ( 1938 ) in a model which has since been applied to epitaxial monolayers ( Frank and van der ...
Page 168
... term contributes only for near neighbors . H ( K ) gives an important contribution in the region between Bragg reflections , if defects have large distortions like interstitials , as shown by Eisenriegler ( 1972 ) recently . The crucial ...
... term contributes only for near neighbors . H ( K ) gives an important contribution in the region between Bragg reflections , if defects have large distortions like interstitials , as shown by Eisenriegler ( 1972 ) recently . The crucial ...
Page 171
... term changes sign for q crossing the Bragg reflection . The scattering patterns in the vicinity of Bragg reflections as they can be determined from the iкs ( K ) term in Eq . ( 62 ) can be very complicated , depending on the anisotropy ...
... term changes sign for q crossing the Bragg reflection . The scattering patterns in the vicinity of Bragg reflections as they can be determined from the iкs ( K ) term in Eq . ( 62 ) can be very complicated , depending on the anisotropy ...
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