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

### From inside the book

Results 1-3 of 77

Page 16

T curve for a

be done accurately . For the heavier rare - earth ions , the maximum obtainable

magnetic moment ( i.e. with no quenching of the orbital angular momentum and

no ...

T curve for a

**given**x would be congruent to the predicted one , and this is yet tobe done accurately . For the heavier rare - earth ions , the maximum obtainable

magnetic moment ( i.e. with no quenching of the orbital angular momentum and

no ...

Page 50

The values of M , ( 0 ) and Mg ( 0 ) are

substitutions in the a- and d - sites , the N , are

of the Gd3 + ions was neglected and the following values of N , used : N 6.0 and

Na ...

The values of M , ( 0 ) and Mg ( 0 ) are

**given**by eqs . ( III - 3.15 ) . Forsubstitutions in the a- and d - sites , the N , are

**given**by eqs . ( III - 3.16 ) . Cantingof the Gd3 + ions was neglected and the following values of N , used : N 6.0 and

Na ...

Page 253

14 is used , the magnetization M at any point will be

independent portion Mo , which describes the orientation of the spins in the

ground state , plus a smaller transverse component m , which is time dependent

and has a ...

14 is used , the magnetization M at any point will be

**given**by a time -independent portion Mo , which describes the orientation of the spins in the

ground state , plus a smaller transverse component m , which is time dependent

and has a ...

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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 |