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

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Page 39

It would be interesting to carry out

the d bands are respectively 4 and 2 eV below E . If we turn now to the transition

metals Ni , Pd and Pt , then the Fermi level intersects the d bands and the ...

It would be interesting to carry out

**similar**calculations for Ag and for Au , wherethe d bands are respectively 4 and 2 eV below E . If we turn now to the transition

metals Ni , Pd and Pt , then the Fermi level intersects the d bands and the ...

Page 312

anomalously large residual resonance resistivity for the alloys with incompletely

filled virtual levels , Fe , Ni such as in Fig . 186 . Figure 24 shows indeed that for a

series of ...

**Similar**results obtain in Co base alloys . In such a model one expectsanomalously large residual resonance resistivity for the alloys with incompletely

filled virtual levels , Fe , Ni such as in Fig . 186 . Figure 24 shows indeed that for a

series of ...

Page 394

It is very

band . From there one can go back to Friedel ' s results . The corresponding

phase shifts nils ) are given by ( 4 ) tg no ( s ) = E + SE – E ' In principle ,

Anderson ' s ...

It is very

**similar**to Stoner ' s criterion for the appearance of ferromagnetism in aband . From there one can go back to Friedel ' s results . The corresponding

phase shifts nils ) are given by ( 4 ) tg no ( s ) = E + SE – E ' In principle ,

Anderson ' s ...

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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