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

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Page 215

This agrees qualitatively with observations : dilute Ni impurity atoms in noble

metals show no localized moment while Cr , Mn , and Fe impurity atoms ... We

first consider a

there .

This agrees qualitatively with observations : dilute Ni impurity atoms in noble

metals show no localized moment while Cr , Mn , and Fe impurity atoms ... We

first consider a

**host metal**with a vacant lattice point and put a 3d impurity atomthere .

Page 229

24 VOLO mo 3 ) When the band of the

induced moments are mostly negative . 4 ) When the number of electrons in the

spin ...

24 VOLO mo 3 ) When the band of the

**host metal**is nearly half - filled , theinduced moments are mostly negative . 4 ) When the number of electrons in the

**host metal**band increases , we have an increasing tendency towards parallelspin ...

Page 249

E n°1 / 2 . mo The self - consistent solutions for this problem may be classified

into the following two categories : i ) There is only one solution for a given

this ...

E n°1 / 2 . mo The self - consistent solutions for this problem may be classified

into the following two categories : i ) There is only one solution for a given

**host****metal**, a given value of E , and a given value of the exchange parameter U . Inthis ...

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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