Proceedings of the International School of Physics "Enrico Fermi.", Volume 70N. Zanichelli, 1978 - Nuclear physics |
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Page 191
... position of the bubble is simply this same equation with If He = 0 and 7 , 0 , we find a remarkable result , namely the final position is μHT , where it would have been according to the simple linear theory , ignoring Bloch - line ...
... position of the bubble is simply this same equation with If He = 0 and 7 , 0 , we find a remarkable result , namely the final position is μHT , where it would have been according to the simple linear theory , ignoring Bloch - line ...
Page 530
... position that the seed is above the melt surface ( position I ) . After spon- taneous nucleation has occurred by slow cooling - the melt is now saturated— the crucible is turned into the growth position ( position II ) , so that the ...
... position that the seed is above the melt surface ( position I ) . After spon- taneous nucleation has occurred by slow cooling - the melt is now saturated— the crucible is turned into the growth position ( position II ) , so that the ...
Page 531
... position I Fig . 9 . - growth position Positions of the crucible for bottom - seeding . 34 Rendiconti S.I.F. LXX end position I a ) b ) Fig . 10. Seed crystal a. 250 g Y , Fe , 012 crystals grown by spontaneous nucleation from a 3 kg ...
... position I Fig . 9 . - growth position Positions of the crucible for bottom - seeding . 34 Rendiconti S.I.F. LXX end position I a ) b ) Fig . 10. Seed crystal a. 250 g Y , Fe , 012 crystals grown by spontaneous nucleation from a 3 kg ...
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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