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

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Page vii

Effect of exchange

Conduction - electron localized moment

dilute alloys .

Effect of exchange

**interaction**in the host metal . . . 230 4 ' 4 ... Energy of**interaction**between two localized moments » 242 5 ' 4 . Critical ... DONIACH –Conduction - electron localized moment

**interaction**in rare - earth metals anddilute alloys .

Page 46

Because electrostatic

Coulomb

range ) , the effect of using a pseudoWannier basis is to reduce the strength ...

Because electrostatic

**interactions**in the metal are screened , so that theCoulomb

**interaction**is replaced by an**interaction**of the Yukawa type ( short -range ) , the effect of using a pseudoWannier basis is to reduce the strength ...

Page 431

Clearly , it would be extremely tedius to solve ( 78 ) for A , construct the total

energy U from ( 82 ) , and then minimize U as a function of Q for a general

the linear ...

Clearly , it would be extremely tedius to solve ( 78 ) for A , construct the total

energy U from ( 82 ) , and then minimize U as a function of Q for a general

**interaction**. Accordingly , we shall find a simple , parametrized form of ve , solvethe linear ...

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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