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 , Fk , 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 , Fk , 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 | |
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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