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

### From inside the book

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Page 22

The purpose of these lectures is to outline in a qualitative way the nature of the d

accurate computations of the

been ...

The purpose of these lectures is to outline in a qualitative way the nature of the d

**bands**and conduction**bands**of ... Within the least five years a number ofaccurate computations of the

**band**structures of many transition metals havebeen ...

Page 288

s d mixing . the more localized d states , and thus brings the d

energy range of the s

that , in general , the crossing of the two

...

s d mixing . the more localized d states , and thus brings the d

**band**within theenergy range of the s

**band**( Fig . 7b ) . Then from symmetry arguments , we knowthat , in general , the crossing of the two

**bands**will be removed by s d mixing , the...

Page 301

9a , b ) , where one half d -

produced by alloying will remove or add electrons mostly to the partially empty

half d -

the ...

9a , b ) , where one half d -

**band**( with spin up ) is full , the shifting of the**bands**produced by alloying will remove or add electrons mostly to the partially empty

half d -

**band**with spin down . In first approximation , the change of population ofthe ...

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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