Proceedings of the International School of Physics "Enrico Fermi.", Volume 70N. Zanichelli, 1978 - Nuclear physics |
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Page 84
Different approaches have been used to calculate the magnitude , sign and
temperature dependence of the anisotropy and magnetostriction constants . The
main attention was paid to the single - ion model permitting the calculation of the
...
Different approaches have been used to calculate the magnitude , sign and
temperature dependence of the anisotropy and magnetostriction constants . The
main attention was paid to the single - ion model permitting the calculation of the
...
Page 117
The theoretical curve ( - ) has been calculated from eq . ( 8.10 ) . AK AK , at T = 0
K has been calculated from 4./2= 1.06 [ 142 ] without any adjustable parameter ;
0.004 , o x = 0.009 , o X = 0.021 . or Ru3 + contribution , when K ( 2 ) and K ( 0 ) ...
The theoretical curve ( - ) has been calculated from eq . ( 8.10 ) . AK AK , at T = 0
K has been calculated from 4./2= 1.06 [ 142 ] without any adjustable parameter ;
0.004 , o x = 0.009 , o X = 0.021 . or Ru3 + contribution , when K ( 2 ) and K ( 0 ) ...
Page 251
Figure 22 shows the calculated temperature dependence of the critical angle
observed in YIG films . The large deviations between the observed and the
calculated behavior could be corrected 90 surface mode 60H critical angle 30
surface ...
Figure 22 shows the calculated temperature dependence of the critical angle
observed in YIG films . The large deviations between the observed and the
calculated behavior could be corrected 90 surface mode 60H critical angle 30
surface ...
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Contents
Magnetooptical rotation | 2 |
Rareearth iron garnets | 5 |
Bubble translation | 8 |
Copyright | |
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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 |