Proceedings of the International School of Physics "Enrico Fermi.", Volume 70N. Zanichelli, 1978 - Nuclear physics |
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Page 380
... polarization . The linear polarizations lie around the equator . Note that orthogonal linear polarizations are at opposite ends of a diameter . Pos- itive circular polarization , i.e. left handed , corresponds to the north pole ...
... polarization . The linear polarizations lie around the equator . Note that orthogonal linear polarizations are at opposite ends of a diameter . Pos- itive circular polarization , i.e. left handed , corresponds to the north pole ...
Page 381
... polarization ellipses encountered along the meridian at 22 : - 45 ° . b ) Poincaré sphere showing the small circle of polarizations which have the same projections on analyzers A and A , as the polarization P. a ) Every polarization ...
... polarization ellipses encountered along the meridian at 22 : - 45 ° . b ) Poincaré sphere showing the small circle of polarizations which have the same projections on analyzers A and A , as the polarization P. a ) Every polarization ...
Page 385
... polarization other than one of the two normal modes , it is resolved onto the normal modes ; these proceed through the crystal with velocities determined by N , and N. As the thickness increases , the resultant polarization on exit is ...
... polarization other than one of the two normal modes , it is resolved onto the normal modes ; these proceed through the crystal with velocities determined by N , and N. As the thickness increases , the resultant polarization on exit is ...
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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