## Proceedings of the International School of Physics "Enrico Fermi.", Volume 70N. Zanichelli, 1978 - Nuclear physics |

### From inside the book

Results 1-3 of 86

Page 166

This

discontinuous stepchange – 298. The value of ' , clearly depends on the location

of Y. If we choose Y to be constant , then it is plausible , as shown rigorously [ 35 ]

...

This

**plane**may , if we so choose , depend on time . Across this cut , y has adiscontinuous stepchange – 298. The value of ' , clearly depends on the location

of Y. If we choose Y to be constant , then it is plausible , as shown rigorously [ 35 ]

...

Page 217

the spin operators from the crystallographic X , Y , Z axes to the axes Y ' ' , Y ' , Z ' ,

where the Z - axis coincides with the spin quantization axis 7 and the Y ' - axis

lies in the ( -X , Y ) -

the spin operators from the crystallographic X , Y , Z axes to the axes Y ' ' , Y ' , Z ' ,

where the Z - axis coincides with the spin quantization axis 7 and the Y ' - axis

lies in the ( -X , Y ) -

**plane**[ 53 ] : ( 4.5 ) Sv = 78 ; + 73 ( 1877 + A * s ;; ) The A ...Page 380

From the

medium , we know that the electric displacement and the magnetic field are

orthogonal to each other and to the direction of propagation . If we consider the

behavior of ...

From the

**plane**- wave solutions of Maxwell's equations for an anisotropicmedium , we know that the electric displacement and the magnetic field are

orthogonal to each other and to the direction of propagation . If we consider the

behavior of ...

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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 |