Treatise on Materials Science and TechnologyHerbert Herman |
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Page 155
... intensity Lopt . For instance in the case of || = 3 Å ̄1 and with AK , 10-4 -4 Å - 2 and disregarding energy resolution this optimum choice would be ko antiparallel to k1 , | ko | = | k1 = 1.5 A - 1 and Ak , 5 x 10-5 A - 2 for every i ...
... intensity Lopt . For instance in the case of || = 3 Å ̄1 and with AK , 10-4 -4 Å - 2 and disregarding energy resolution this optimum choice would be ko antiparallel to k1 , | ko | = | k1 = 1.5 A - 1 and Ak , 5 x 10-5 A - 2 for every i ...
Page 186
Herbert Herman. RELATIVE INTENSITY ( arbitrary scale ) 20 20 16 2 T 1.0 1.2 BRILLOUIN ZONE BOUNDARY 1.4 1.6 CALCULATED Cu - 4 % Al Cu - 10 % Al 1.8 2.0 9 COMPONENT ( in units of 2π / a ) -x Fig . 21. Integrated intensity of localized ...
Herbert Herman. RELATIVE INTENSITY ( arbitrary scale ) 20 20 16 2 T 1.0 1.2 BRILLOUIN ZONE BOUNDARY 1.4 1.6 CALCULATED Cu - 4 % Al Cu - 10 % Al 1.8 2.0 9 COMPONENT ( in units of 2π / a ) -x Fig . 21. Integrated intensity of localized ...
Page 222
... intensity is higher than for q antiparallel to Thkl as observed in the experiment . A more detailed theoretical discussion of Huang scattering by dislocation loops and defect clusters is given by Dederichs ( 1971 ) . Recently an X - ray ...
... intensity is higher than for q antiparallel to Thkl as observed in the experiment . A more detailed theoretical discussion of Huang scattering by dislocation loops and defect clusters is given by Dederichs ( 1971 ) . Recently an X - ray ...
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 R₁ 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 thermal thickness transition metal values vector X-ray YGaG νμ ΦΩ