## Proceedings of the International School of Physics "Enrico Fermi.", Volume 37N. Zanichelli, 1967 - Nuclear physics |

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Page 233

When the impurity moment is sufficiently large , it is not influenced much by the

additional local

perturbation is already large and is in a saturation range . Therefore we may ...

When the impurity moment is sufficiently large , it is not influenced much by the

additional local

**magnetic**field since the effective field at the impurity atom withoutperturbation is already large and is in a saturation range . Therefore we may ...

Page 336

Before discussing the nature and magnitude of these moments and their

interaction with the atomic electrons in some detail we note certain restrictions on

the allowed orders of electric and

by ...

Before discussing the nature and magnitude of these moments and their

interaction with the atomic electrons in some detail we note certain restrictions on

the allowed orders of electric and

**magnetic**multipole moments that are imposedby ...

Page 414

Penn ' s theory of the stability of

transition metals . 3 ' 1 . Introduction . – Excepting the rare - earth metals and

possibly uranium , magnetism in metals occurs only among the trasition metals ,

or alloys ...

Penn ' s theory of the stability of

**magnetic**phases for a simple model of thetransition metals . 3 ' 1 . Introduction . – Excepting the rare - earth metals and

possibly uranium , magnetism in metals occurs only among the trasition metals ,

or alloys ...

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### Contents

LOMER Band theory and magnetism | 1 |

PHILLIPS Band theory of transition metals | 22 |

JACCARINO Studies of the hyperfine interaction in transi | 39 |

Copyright | |

19 other sections not shown

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### Common terms and phrases

alloys appearance approximation assume average band becomes bound boundary calculation charge complex computed condition conduction consider contribution correct correlation corresponding coupling curve defined density depends determined direction discussed effect electrons energy equation exchange existence expected expression fact factor Fermi Fermi level Fermi surface ferromagnetic field function given gives Hamiltonian host metal impurity atom increases integral interaction interesting lattice limit localized magnetic matrix elements means method moments normal Note observed obtained occur operator orbital perturbation phase Phys physical plane polarization poles positive possible potential present problem properties range relation replaced represent resonance scattering screening Sect shift shown similar simple single solution spin strong structure temperature theory tion transition metals usual wave wave functions write zero