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
angle anisotropy Appl approximation assumed atoms average axis c-sites calculated cations coherent concentration condition considerations constant contribution corresponding crystal curve defect density dependence determined diffusion direction discussed dislocations displacement effect elastic elastic scattering electron energy equation et al exist experimental experiments factor field flux lines follows force function garnet given gives important increasing interaction interface ions lattice length Lett limit magnetic materials measured Merwe metal method misfit mode neutron normal obtained parameter phase phonon Phys plane position potential present properties range rare earth reference region relation resolution respectively sample scattering cross section shown shows single solid solution space strain stress structure substrate superconducting surface Table temperature tetrahedral theory thermal thickness transition unit values vector X-ray