Treatise on Materials Science and TechnologyHerbert Herman |
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Page 339
... Anisotropy The magnetization vector M in a ferrimagnetic material is always bound to a certain preferred crystallographic direction , which is the easy axis . Anisotropy energy , F1 , is required to turn M from the easy axis direction ...
... Anisotropy The magnetization vector M in a ferrimagnetic material is always bound to a certain preferred crystallographic direction , which is the easy axis . Anisotropy energy , F1 , is required to turn M from the easy axis direction ...
Page 347
... anisotropy . The orthorhombic anisotropy implies that the Z1 - Z2 population difference is as important as the Z- ( X , Y ) difference . The site population ratios vary approximately exponentially with Ar , where Ar is the excess of the ...
... anisotropy . The orthorhombic anisotropy implies that the Z1 - Z2 population difference is as important as the Z- ( X , Y ) difference . The site population ratios vary approximately exponentially with Ar , where Ar is the excess of the ...
Page 366
... anisotropy implies that there is an anisotropy in the absorption of light by a single set of crystallographic sites . This is a photoinduced dichroism ( Dillon et al . , 1970 ) . For a crystal plate thickness of 0.011 cm , the dichroism ...
... anisotropy implies that there is an anisotropy in the absorption of light by a single set of crystallographic sites . This is a photoinduced dichroism ( Dillon et al . , 1970 ) . For a crystal plate thickness of 0.011 cm , the dichroism ...
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