Proceedings of the International School of Physics "Enrico Fermi.", Volume 70N. Zanichelli, 1978 - Nuclear physics |
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Page 159
... consider any linear transformation R , independent of r , such that M ' ( r ) = ( Ř · M ) , = Σ R , M , ( r ) is a new distribution generated from M ( r ) . Since eq . ( 5.1 ) is linear , M ' ( r ) also satisfies it . To preserve the ...
... consider any linear transformation R , independent of r , such that M ' ( r ) = ( Ř · M ) , = Σ R , M , ( r ) is a new distribution generated from M ( r ) . Since eq . ( 5.1 ) is linear , M ' ( r ) also satisfies it . To preserve the ...
Page 166
... consider Bloch points ) , and eqs . ( 6.6 ) - ( 6.8 ) are am- biguous . Since the observable wall - surface moment is continuous everywhere on the wall , the discontinuity of cannot have any physical consequence . Its occurrence is ...
... consider Bloch points ) , and eqs . ( 6.6 ) - ( 6.8 ) are am- biguous . Since the observable wall - surface moment is continuous everywhere on the wall , the discontinuity of cannot have any physical consequence . Its occurrence is ...
Page 184
... Consider a cylindrical bubble with radius r moving with velocity V parallel to the x - axis , as shown in fig . 41. Let the origin of the moving co - ordinate system lie on the axis of the cylinder . The co - ordinate z and the angular ...
... Consider a cylindrical bubble with radius r moving with velocity V parallel to the x - axis , as shown in fig . 41. Let the origin of the moving co - ordinate system lie on the axis of the cylinder . The co - ordinate z and the angular ...
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absorption angle anisotropy constants antiferromagnetic Appl axis birefringence Bloch lines Bloch point bubble calculated cation cm-¹ Co² Co³ coefficient concentration contribution crystal field cubic Curie temperature curve diamagnetic dichroism direction of magnetization domain wall effects electron energy levels equations exchange experimental Fe2+ Fe³ ferrimagnetic ferromagnetic resonance film formula unit frequency GELLER GILLEO given Hamiltonian interaction ion moments Journ K₁ lattice constant line width linear magnetic anisotropy magnetic field magneto-optical magnetoelastic magnons measurements modes neutron diffraction observed obtained octahedral octahedral sites optical orbital oxygen paramagnetic parameters phonons photoinduced photomagnetic Phys polarization polycrystalline properties rare-earth ions rare-earth iron garnets relaxation resonance room temperature rotation sample shown in fig sin² specimens spin wave spin-orbit coupling spontaneous magnetization sublattice substitution surface symmetry temperature dependence tetrahedral theory tion torque transitions uniaxial anisotropy valence values vector velocity yttrium iron garnet