Proceedings of the International School of Physics "Enrico Fermi.", Volume 70N. Zanichelli, 1978 - Nuclear physics |
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Page 28
In ( III - 3.10 ) , ng is the number of Bohr magnetons per formula unit . Actually ,
this did not fit the results very well , because it predicted rather large occupancies
of the tetrahedral sites by Se3 + and In3 + ions [ 77 ] . Following our earlier work ...
In ( III - 3.10 ) , ng is the number of Bohr magnetons per formula unit . Actually ,
this did not fit the results very well , because it predicted rather large occupancies
of the tetrahedral sites by Se3 + and In3 + ions [ 77 ] . Following our earlier work ...
Page 150
Equations ( 3.5 ) - ( 3.7 ) for surface energy o and wall thickness will require
adjustment to account for curvature . In order to derive equations pertaining to
this surface from the Landau - Lifshitz equations pertaining to a unit volume , we
need to ...
Equations ( 3.5 ) - ( 3.7 ) for surface energy o and wall thickness will require
adjustment to account for curvature . In order to derive equations pertaining to
this surface from the Landau - Lifshitz equations pertaining to a unit volume , we
need to ...
Page 173
From these equations follow the useful relations ( 7.2 ) - 1.4x = 1.4 . sin y Taking a
unit length of Bloch line in this geometry we write ( 7.3 ) w = foda , where the
integral extends to large fixed distances on both sides of X. By applying the chain
...
From these equations follow the useful relations ( 7.2 ) - 1.4x = 1.4 . sin y Taking a
unit length of Bloch line in this geometry we write ( 7.3 ) w = foda , where the
integral extends to large fixed distances on both sides of X. By applying the chain
...
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Contents
Magnetooptical rotation | 2 |
Rareearth iron garnets | 5 |
Bubble translation | 8 |
Copyright | |
35 other sections not shown
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Common terms and phrases
absorption angle anisotropy Appl applied assumed axis Bloch lines bubble calculated causes centres composition consider constants contribution corresponding coupling crystal cubic curve dependence determined direction discussed distribution domain effects electron energy equation exchange experiment experimental expression Fe2+ Fe3+ ions ferrimagnetic field film function GELLER give given ground increases interaction iron garnets Journ lattice levels light magnetic field magnitude material measurements mode moments motion normal observed obtained occur octahedral orientation parallel parameter photoinduced Phys plane polarization position properties rare-earth ions region relation relaxation represents resonance respectively rotation sample shown in fig shows space group specimens spin wave spontaneous spontaneous magnetization structure sublattice substitution surface symmetry temperature tetrahedral theory tion torque transition uniaxial unit values variation wall yttrium iron garnet
References to this book
Structural and Magnetic Phase Transitions in Minerals S. Ghose,J.M.D. Coey,E. Salje Snippet view - 1988 |