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

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Page 207

Therefore it is necessary to describe , in some way or other , the state of the

discuss this problem have been presented by ANDERSON [ 8 ] and by WOLFF [ 9

] ...

Therefore it is necessary to describe , in some way or other , the state of the

**impurity atom**and the interaction between electrons explicitly . Simple models todiscuss this problem have been presented by ANDERSON [ 8 ] and by WOLFF [ 9

] ...

Page 215

This agrees qualitatively with observations : dilute Ni

metals show no localized moment while Cr , Mn , and Fe

localized moments in all noble metals . iii ) When the localized spin moment does

...

This agrees qualitatively with observations : dilute Ni

**impurity atoms**in noblemetals show no localized moment while Cr , Mn , and Fe

**impurity atoms**showlocalized moments in all noble metals . iii ) When the localized spin moment does

...

Page 246

What we see from this figure is : i ) When the

filled d - shells , the interaction between ... one as is expected from the results in

the preceding Section . ii ) When the number of electrons in the

What we see from this figure is : i ) When the

**impurity atoms**have nearly half -filled d - shells , the interaction between ... one as is expected from the results in

the preceding Section . ii ) When the number of electrons in the

**impurity atom**is ...### What people are saying - Write a review

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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 | |

25 other sections not shown

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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