Proceedings of the International School of Physics "Enrico Fermi.", Volume 70N. Zanichelli, 1978 - Nuclear physics |
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Page 150
Equations ( 3.5 ) - ( 3.7 ) for surface energy o and wall thickness will require
adjustment to account for curvature . ... According to the Landau - Lifshitz
equation with Gilbert damping , the components of precession rate 0 , y sin 0 are
related to ...
Equations ( 3.5 ) - ( 3.7 ) for surface energy o and wall thickness will require
adjustment to account for curvature . ... According to the Landau - Lifshitz
equation with Gilbert damping , the components of precession rate 0 , y sin 0 are
related to ...
Page 167
fundamental equation of motion for a closed domain of general shape and
general s . Note that , if we choose the cuts to move with the domain , then the
last term of this equation represents a Lorentz - like force tending to deflect it .
Since cuts ...
fundamental equation of motion for a closed domain of general shape and
general s . Note that , if we choose the cuts to move with the domain , then the
last term of this equation represents a Lorentz - like force tending to deflect it .
Since cuts ...
Page 270
Magnetizing processes and the equation of motion . - When the magnetic field
applied to a sample is changed the magnetization changes in response , relaxing
in a short time to a new equilibrium configuration . We are concerned with the ...
Magnetizing processes and the equation of motion . - When the magnetic field
applied to a sample is changed the magnetization changes in response , relaxing
in a short time to a new equilibrium configuration . We are concerned with 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 |