Proceedings of the International School of Physics "Enrico Fermi.", Volume 70N. Zanichelli, 1978 - Nuclear physics |
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Page 225
The high - field mode is a surface mode localized at the substrate interface of the
film ( ref . [ 37 ] ) . surface impurities removed and yield a natural pinning
condition , A , = 1 , at that surface . In this manner the properties of the magnetic ...
The high - field mode is a surface mode localized at the substrate interface of the
film ( ref . [ 37 ] ) . surface impurities removed and yield a natural pinning
condition , A , = 1 , at that surface . In this manner the properties of the magnetic ...
Page 227
Spin wave spectra showing the first two high - field modes in the parallel
orientation as a function of temperature for a YIG film having a single surface
mode at room temperature ( ref . [ 37 ] ) . at 740 , 900 , 1000 , 1100 and 1200 ° C .
Each line ...
Spin wave spectra showing the first two high - field modes in the parallel
orientation as a function of temperature for a YIG film having a single surface
mode at room temperature ( ref . [ 37 ] ) . at 740 , 900 , 1000 , 1100 and 1200 ° C .
Each line ...
Page 286
This illustrates very clearly that the anisotropy broadening is due to scattering of
the uniform mode into degenerate spin waves of low k value , because for l < }
the uniform mode is no longer degenerate with such modes : when Q = } the ...
This illustrates very clearly that the anisotropy broadening is due to scattering of
the uniform mode into degenerate spin waves of low k value , because for l < }
the uniform mode is no longer degenerate with such modes : when Q = } the ...
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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 |