Treatise on Materials Science and TechnologyHerbert Herman |
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Page 109
... angle is the angle between ko 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 scattering length a is ...
... angle is the angle between ko 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 scattering length a is ...
Page 215
... ANGLE SCATTERING AT t = 0 Between 1957 and 1960 in a period of growing importance of X - ray small angle scattering the discovery of double Bragg scattering as a parasitic scatter- ing process caused a sudden stop . For a 1.54 Å X - ray ...
... ANGLE SCATTERING AT t = 0 Between 1957 and 1960 in a period of growing importance of X - ray small angle scattering the discovery of double Bragg scattering as a parasitic scatter- ing process caused a sudden stop . For a 1.54 Å X - ray ...
Page 217
... angle scattering a quadratic pattern if the incident neutron beam is parallel to the precipitation Fig . 41. Photograph of neutron small angle scattering from Ticonal ( by courtesy of J. Lerch ) . White areas are neutron intense regions ...
... angle scattering a quadratic pattern if the incident neutron beam is parallel to the precipitation Fig . 41. Photograph of neutron small angle scattering from Ticonal ( by courtesy of J. Lerch ) . White areas are neutron intense regions ...
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