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

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Page 206

Institute for Solid State Physics , University of Tokyo - Acabu , Tokyo 1 . -

Introduction . The problem of

subject of ...

**Localized**Magnetic Moments in Transition Metals and Alloys . T . MORIYAInstitute for Solid State Physics , University of Tokyo - Acabu , Tokyo 1 . -

Introduction . The problem of

**localized**magnetic moments in metals has been asubject of ...

Page 207

In the problem of

interaction between the electrons , and the impurity potential must be determined

self - consistently , in a Hartree - Fock sense . Therefore it is necessary to ...

In the problem of

**localized**magnetic moments it is essential to take account of theinteraction between the electrons , and the impurity potential must be determined

self - consistently , in a Hartree - Fock sense . Therefore it is necessary to ...

Page 252

As has been discussed in the preceding Sections the physical picture of the

ferromagnetic ...

As has been discussed in the preceding Sections the physical picture of the

**localized**virtual states and the usefulness of this concept in discussing the**localized**- moment problem are clear in dilute alloys , either paramagnetic orferromagnetic ...

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### Contents

LOMER Band theory and magnetism | 1 |

JACCARINO Studies of the hyperfine interaction in transi | 39 |

P W ANDERSON and W L MCMILLAN Multiplescattering | 50 |

Copyright | |

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### Common terms and phrases

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