Proceedings of the International School of Physics "Enrico Fermi.", Volume 70N. Zanichelli, 1978 - Nuclear physics |
From inside the book
Results 1-3 of 66
Page 31
3 ; b ) until the transition points are reached , although the rates of decrease of
effective moments with increasing w are ... c ) the transitions for a - site
substitution occur at a much lower value of x than for d - site substitution ; d ) the
transition for ...
3 ; b ) until the transition points are reached , although the rates of decrease of
effective moments with increasing w are ... c ) the transitions for a - site
substitution occur at a much lower value of x than for d - site substitution ; d ) the
transition for ...
Page 449
In essence it is simple to distinguish between an isolated diamagnetic or
paramagnetic transition . In Y , Fe , 012 , due to many overlapping components ,
interpretation is aided by a determination of both & and & line shapes . 3 .
Absorption ...
In essence it is simple to distinguish between an isolated diamagnetic or
paramagnetic transition . In Y , Fe , 012 , due to many overlapping components ,
interpretation is aided by a determination of both & and & line shapes . 3 .
Absorption ...
Page 459
to the low - frequency refractive index originates ; this region is attributed to
allowed interband 2p - 48 transitions . ... The origin of this region is most likely the
allowed interconfigurational transition 3ds → 3d * 4p of Fe3 + which is known to ...
to the low - frequency refractive index originates ; this region is attributed to
allowed interband 2p - 48 transitions . ... The origin of this region is most likely the
allowed interconfigurational transition 3ds → 3d * 4p of Fe3 + which is known to ...
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 |