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

### From inside the book

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Page 39

Thus we must 1.07 rely on Fermi surface data to fix the position of the d bands and

Thus we must 1.07 rely on Fermi surface data to fix the position of the d bands and

**conduction**bands . 1.03 In the nonmagnetic metals Pd and Pt the ...Page 226

The total change in the number of

The total change in the number of

**conduction**electrons due to the covalent admixture with the impurity atom is given by EF ( 4.4 ) dng = de docond ( e ) ...Page 261

where r COS - sin x ( 1.22 ) Fr ) and Q , is the

where r COS - sin x ( 1.22 ) Fr ) and Q , is the

**conduction**electron density . Similarly for Qj ( r ) with f → -f . Thus the total charge density exte ...### 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