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

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Page 38

obtained by studying de Haas - van Alphen oscillations in the magnetic susceptibility ; from the periods of these oscillations extremal cross - sectional areas of the

obtained by studying de Haas - van Alphen oscillations in the magnetic susceptibility ; from the periods of these oscillations extremal cross - sectional areas of the

**Fermi**surface can be determined . Several experimental techniques ...Page 39

It would be interesting to carry out similar calculations for Ag and for Au , where the d bands are respectively 4 and 2 eV below Er . If we turn now to the transition metals Ni , Pd and Pt , then 1.15 the

It would be interesting to carry out similar calculations for Ag and for Au , where the d bands are respectively 4 and 2 eV below Er . If we turn now to the transition metals Ni , Pd and Pt , then 1.15 the

**Fermi**level intersects the d ...Page 47

Because the d bands lie closer to the

Because the d bands lie closer to the

**Fermi**energy , the interband transitions are superposed on a large Drude background , and hence are less easily resolved . Structure has been identified [ 55 ] in the infrared at 0.3 eV with weaker ...### 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 | |

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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