## 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 |

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