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

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Page 228

Parallel - spin

Parallel - spin

**polarization**is possible for ( E. – Ez ) / w < 0.2 ~ 0.3 . Since the value of ( E.1 – Eor ) cannot be too large , the range of parallel ...Page 229

9 . atom increases , we have an increasing tendency towards parallel spin

9 . atom increases , we have an increasing tendency towards parallel spin

**polarization**. 1.0 1.0 0.8 0.8 0.2 1.8 1.9 1.6 1.4 18,0.2 1.6.0.4 1.4 , 0.6 1.2 ...Page 235

Fermi surface is required in order to calculate the spatial distribution of the spin

Fermi surface is required in order to calculate the spatial distribution of the spin

**polarization**. The exchange interaction in the host metal gives further ...### 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