Treatise on Materials Science and TechnologyHerbert Herman |
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Page 124
... vector q is defined by K = Thkl + q ( II.73 ) The vector q is restricted to the first Brillouin zone . For a fixed к , there is only a contribution if the energy transfer ho is equal to one of the h @ ph , j of the different phonon ...
... vector q is defined by K = Thkl + q ( II.73 ) The vector q is restricted to the first Brillouin zone . For a fixed к , there is only a contribution if the energy transfer ho is equal to one of the h @ ph , j of the different phonon ...
Page 158
Herbert Herman. position vector R = 0. We obtain a scattering length bo ° of the defect at R1 = 0 and new position vectors for the host lattice atoms R , = R1 ° + s1 • The vectors s , are the distortion vectors originated by the defect ...
Herbert Herman. position vector R = 0. We obtain a scattering length bo ° of the defect at R1 = 0 and new position vectors for the host lattice atoms R , = R1 ° + s1 • The vectors s , are the distortion vectors originated by the defect ...
Page 182
... vectors interconnecting Fermi surface . Positron annihilation experiments ( Fujiwara et al . , 1968 ) sensing electron K - vector densities also are in good agreement with the X - ray data . It is the author's impression that the ...
... vectors interconnecting Fermi surface . Positron annihilation experiments ( Fujiwara et al . , 1968 ) sensing electron K - vector densities also are in good agreement with the X - ray data . It is the author's impression that the ...
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