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

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Page 30

Near the

Near the

**resonance**energy Em , y assumes the form [ 21 ] KW " ( 2.17 ) Y'res lice rom a EW ) 2 + II ? where the factor K occurs because y is normalized by ...Page 31

Again we transform by ( 2.6 ) to rewrite the second term of ( 2.21 ) as ( 2.22 ) – ( E- E'Y ) KOM Far from

Again we transform by ( 2.6 ) to rewrite the second term of ( 2.21 ) as ( 2.22 ) – ( E- E'Y ) KOM Far from

**resonance**tg na — sin n . so that we may combine ...Page 199

Evidently we always get a

Evidently we always get a

**resonance**, in 1-2 or et à according as g 2 ) is ferromagnetic ( 0 ) or antiferromagnetic ( > 0 ) . To obtain a qualitative notion ...### 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