Proceedings of the International School of Physics "Enrico Fermi.", Volume 70N. Zanichelli, 1978 - Nuclear physics |
From inside the book
Results 1-3 of 91
Page 210
Returning to the diagonalized Hamiltonian , eq . ( 2.27 ) , the coefficient to the
bilinear terms determines the spin wave dispersion relation . By substituting for
the values of Ay and B. in eq . ( 2.18 ) , the dispersion relation takes the form i i (
2.30 ) ...
Returning to the diagonalized Hamiltonian , eq . ( 2.27 ) , the coefficient to the
bilinear terms determines the spin wave dispersion relation . By substituting for
the values of Ay and B. in eq . ( 2.18 ) , the dispersion relation takes the form i i (
2.30 ) ...
Page 238
The dispersion relation from eq . ( 5.19 ) then yields 0 ( 5.21 ) Dki H.- HK r and the
ellipticity from eqs . ( 5.18 ) gives ( 5.22 ) 818 B2 B. i , Blå a circular precession as
expected . When the magnetization is oriented in the plane of the film , where ...
The dispersion relation from eq . ( 5.19 ) then yields 0 ( 5.21 ) Dki H.- HK r and the
ellipticity from eqs . ( 5.18 ) gives ( 5.22 ) 818 B2 B. i , Blå a circular precession as
expected . When the magnetization is oriented in the plane of the film , where ...
Page 244
Setting EQ = 0 with 0 = 1/2 yields the relation ( 5.49 ) M , H , sin ( Q - 9 + 1 + 20 M
; sin 2q + K , sin 29 ( 1 – 7 cos 20 ) + cos ? 9 ( 2 cos 20 3 al -1 ) ] = 0 0 . There is in
general no analytic solution to this equation and it will be carried in this form ...
Setting EQ = 0 with 0 = 1/2 yields the relation ( 5.49 ) M , H , sin ( Q - 9 + 1 + 20 M
; sin 2q + K , sin 29 ( 1 – 7 cos 20 ) + cos ? 9 ( 2 cos 20 3 al -1 ) ] = 0 0 . There is in
general no analytic solution to this equation and it will be carried in this form ...
What people are saying - Write a review
We haven't found any reviews in the usual places.
Contents
Magnetooptical rotation | 2 |
Rareearth iron garnets | 5 |
Bubble translation | 8 |
Copyright | |
35 other sections not shown
Other editions - View all
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 |
Bibliographic information
| Title | Proceedings of the International School of Physics "Enrico Fermi.", Volume 70 Proceedings of the International School of Physics "Enrico Fermi.", Società italiana di fisica Rivista del nuovo cimento |
| Contributor | Società italiana di fisica |
| Publisher | N. Zanichelli, 1978 |
| Original from | the University of California |
| Digitized | 13 Aug 2008 |
| ISBN | 044485200X, 9780444852007 |
| Export Citation | BiBTeX EndNote RefMan |