Treatise on Materials Science and TechnologyHerbert Herman |
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Page 260
... applied field approaches H. 2 , the formation of the corresponding FLD does not seem to be too difficult , and a fluidlike structure should develop near H. 2 ( Labusch , 1969a ) . On the other hand , recent neutron diffraction ...
... applied field approaches H. 2 , the formation of the corresponding FLD does not seem to be too difficult , and a fluidlike structure should develop near H. 2 ( Labusch , 1969a ) . On the other hand , recent neutron diffraction ...
Page 337
... applied to ferrimagnetism ( Néel , 1948 ) , shows that the fields acting at a- , d- , and c - sites , respectively , are - H1 = H – Naa Ma - Nad Md - Nac Mc Ha H1 = H - NdaMa - Ha H1 = H- Nea Ma Nad Ma - Nde Mc dd d dc Ned Md - Nec M ...
... applied to ferrimagnetism ( Néel , 1948 ) , shows that the fields acting at a- , d- , and c - sites , respectively , are - H1 = H – Naa Ma - Nad Md - Nac Mc Ha H1 = H - NdaMa - Ha H1 = H- Nea Ma Nad Ma - Nde Mc dd d dc Ned Md - Nec M ...
Page 366
... applied there is a certain period of time during which no flux is switched irreversibly . The level of this delay depends on the amplitude of the applied step field . After this delay , the YIG : Si switches in the normal way . At 4.2 ...
... applied there is a certain period of time during which no flux is switched irreversibly . The level of this delay depends on the amplitude of the applied step field . After this delay , the YIG : Si switches in the normal way . At 4.2 ...
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 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 tetrahedral thermal thickness transition metal values vector X-ray YGaG