Treatise on Materials Science and TechnologyHerbert Herman |
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Page 109
... rays . The scattering angle is the angle between k 。 and k1 , and is the azimuthal angle . Neutron wavelengths between 0.5 and 20 Å are used . A comparison with nuclear dimensions , which are of the order of 10-5 Å , shows that the ...
... rays . The scattering angle is the angle between k 。 and k1 , and is the azimuthal angle . Neutron wavelengths between 0.5 and 20 Å are used . A comparison with nuclear dimensions , which are of the order of 10-5 Å , shows that the ...
Page 146
... rays beam extraction is much simpler . However , for special cases like backscattering experiments or possibly for multiple use of a rotating anode an X - ray guide tube technique may be considered also . Both in X - ray and neutron ...
... rays beam extraction is much simpler . However , for special cases like backscattering experiments or possibly for multiple use of a rotating anode an X - ray guide tube technique may be considered also . Both in X - ray and neutron ...
Page 177
... RAYS : σabs ( 4Å ) + σ Inc 4π02 ( K ) absorption Fig . 18. Two - dimensional diagram for suitability of various ... rays with к as parameter . K - values can be read from the table inserted in the figure . if σinc is small . For X rays ...
... RAYS : σabs ( 4Å ) + σ Inc 4π02 ( K ) absorption Fig . 18. Two - dimensional diagram for suitability of various ... rays with к as parameter . K - values can be read from the table inserted in the figure . if σinc is small . For X rays ...
Contents
Epitaxial Interfaces | 3 |
Thin Films | 15 |
Semiinfinite Overgrowths | 37 |
Copyright | |
13 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 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