Treatise on Materials Science and TechnologyHerbert Herman |
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Page 158
... 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 . We set s , ( R , ° = 0 ) = 0 , a condition obvious for a normal substitutional ...
... 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 . We set s , ( R , ° = 0 ) = 0 , a condition obvious for a normal substitutional ...
Page 171
... DEFECTS From a first glance at the literature sufficient experimental data of substi- tutional alloys would be expected , allowing both defect arrangement and displacement field around individual substitutional atoms to be deduced . As ...
... DEFECTS From a first glance at the literature sufficient experimental data of substi- tutional alloys would be expected , allowing both defect arrangement and displacement field around individual substitutional atoms to be deduced . As ...
Page 172
... defect induced change in total cross section and the angular dependence of the scattering cross section have been used as an indication for defect clusters ( BeO ) , for amorphous zones ( SiO2 ) , and for point defects or very small ...
... defect induced change in total cross section and the angular dependence of the scattering cross section have been used as an indication for defect clusters ( BeO ) , for amorphous zones ( SiO2 ) , and for point defects or very small ...
Contents
Epitaxial Interfaces | 3 |
Thin Films | 15 |
Semiinfinite Overgrowths | 37 |
Copyright | |
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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