Treatise on Materials Science and TechnologyHerbert Herman |
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Page 168
... defects is assumed . The Fourier transform in the correction term contributes only for near neighbors . H ( K ) gives an important contribution in the region between Bragg reflections , if defects have large distortions like ...
... defects is assumed . The Fourier transform in the correction term contributes only for near neighbors . H ( K ) gives an important contribution in the region between Bragg reflections , if defects have large distortions like ...
Page 171
... defect clusters where the same formalism can be used as shown by Dederichs ( 1971 ) . In practice however one is confronted with two averaging processes : ( i ) Anisotropic defects are often distributed with their preferential axes ...
... defect clusters where the same formalism can be used as shown by Dederichs ( 1971 ) . In practice however one is confronted with two averaging processes : ( i ) Anisotropic defects are often distributed with their preferential axes ...
Page 187
... DEFECTS For MD > MH the defect mode remains in the host lattice phonon band and is called a resonance mode with characteristic frequency @R . The phonon dispersion curve is changed with o in a way typical of resonance phenomena . For ...
... DEFECTS For MD > MH the defect mode remains in the host lattice phonon band and is called a resonance mode with characteristic frequency @R . The phonon dispersion curve is changed with o in a way typical of resonance phenomena . For ...
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