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

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Page 166

This

discontinuous stepchange – 27 S. The value of 'P', clearly depends on the

location of Y. If we choose Y to be constant, then it is plausible, as shown

rigorously [35], that ...

This

**plane**may, if we so choose, depend on time. Across this cut, op has adiscontinuous stepchange – 27 S. The value of 'P', clearly depends on the

location of Y. If we choose Y to be constant, then it is plausible, as shown

rigorously [35], that ...

Page 217

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

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

the (X, Y)-

following ...

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

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

the (X, Y)-

**plane**[53]: -- - 1 r r (4.5) S.-ys sas, 4's). The A vector satisfies thefollowing ...

Page 380

From the

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 D ...

From the

**plane**-wave solutions of Maxwell's equations for an anisotropic 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 D ...

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### Contents

Gruppo fotografico dei partecipanti al Corso fuori testo | 1 |

Octahedral sites | 3 |

Hightemperature results | 4 |

Copyright | |

34 other sections not shown

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### Common terms and phrases

absorption angle anisotropy constants anisotropy energy annealing antiferromagnetic Appl axis Bloch lines Bloch point Bloch wall Bloch-line bubble calculated coefficients compensation point contribution Cošt crystal field cubic Curie temperature curve d-site diamagnetic dichroism direction of magnetization domain wall effects electron energy levels equation exchange experimental Fe2+ Fe3+ ions ferromagnetic resonance formula unit frequency gadolinium Gd3+ ion GELLER GILLEo given Hamiltonian interaction ion moments Journ lattice constant line width linear magnetic field magnetic ions magnetoelastic magnetostriction constants measurements neutron diffraction observed octahedral octahedral sites orientation parameter phonons photoinduced photomagnetic Phys plane polarization rare-earth ions rare-earth iron garnets relaxation respectively room temperature rotation sample shown in fig specimens spin wave spontaneous magnetization sublattice substitution symmetry temperature dependence temperature variation tetrahedral theory tion torque transition uniaxial anisotropy valence values vector velocity yttrium iron garnet