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

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Page 186

In fact it sharpens and moves towards the Fermi level from above , as the

standard , provided we assume Mathiesorward sen ' s rule : that one may simply

add up ...

In fact it sharpens and moves towards the Fermi level from above , as the

**temperature**KT is decreased . The calculation of the transport properties isstandard , provided we assume Mathiesorward sen ' s rule : that one may simply

add up ...

Page 270

Comparison of ( 1 . 62 ) with the Curie '

not expected to be strongly

) .

Comparison of ( 1 . 62 ) with the Curie '

**temperatures**extrapolated from high**temperatures**( 1 . ... 46 ) should in this theory not vary with**temperature**, as X , isnot expected to be strongly

**temperature**- dependent in the approximation ( 1 . 37) .

Page 271

However in this part we continue with the localized spin model used in a

phenomenological way and discuss how much use the model is in correlating

properties of the dilute alloys . 2 ' 1 . Paramagnetic Curie

However in this part we continue with the localized spin model used in a

phenomenological way and discuss how much use the model is in correlating

properties of the dilute alloys . 2 ' 1 . Paramagnetic Curie

**temperatures**...### 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