Proceedings of the International School of Physics "Enrico Fermi.", Volume 70N. Zanichelli, 1978 - Nuclear physics |
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Page 380
Ellipticities of +1 and — 1 correspond to left and right circularly polarized light .
An ellipticity of 0 designates ... Any polarization state could be specified with 2 in
the range 0 to n and with w in the range 2/4 to + 2/4 . The Poincaré - sphere ...
Ellipticities of +1 and — 1 correspond to left and right circularly polarized light .
An ellipticity of 0 designates ... Any polarization state could be specified with 2 in
the range 0 to n and with w in the range 2/4 to + 2/4 . The Poincaré - sphere ...
Page 382
A familiar and important example of this is the addition of right- and left - hand
circular polarized light in equal intensities to produce a linear polarization . The
two normal polarizations are the north and south pole of the sphere , and the ...
A familiar and important example of this is the addition of right- and left - hand
circular polarized light in equal intensities to produce a linear polarization . The
two normal polarizations are the north and south pole of the sphere , and the ...
Page 385
An initial linear polarization would become elliptical with the same azimuth of its
major axis . For light traveling along a direction perpendicular to M , say [ 100 ] ,
we can readily follow a similar procedure and find that , for Es , N , = Vazz and ,
for ...
An initial linear polarization would become elliptical with the same azimuth of its
major axis . For light traveling along a direction perpendicular to M , say [ 100 ] ,
we can readily follow a similar procedure and find that , for Es , N , = Vazz and ,
for ...
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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 |