## 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

must allow for the rapid

section ...

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

**temperature**KT is decreased . ... Its displacement from £ , reflects conditions notmust allow for the rapid

**variation**of the tied to the vicinity of Ep . collision cross -section ...

Page 270

62 ) with the Curie ' temperatures extrapolated from high temperatures ( 1 . ... The

low -

18 ] in terms of what amounts to an RKY potential calculated beyond second ...

62 ) with the Curie ' temperatures extrapolated from high temperatures ( 1 . ... The

low -

**temperature variation**has been discussed by ELLIOTT and WEDGWOOD [18 ] in terms of what amounts to an RKY potential calculated beyond second ...

Page 272

3 ) c = Nim / N . Hence , within this model , we have in the high

22 ] ( 2 . ... density of states giving an additional susceptibitlity which

with

3 ) c = Nim / N . Hence , within this model , we have in the high

**temperature**limit [22 ] ( 2 . ... density of states giving an additional susceptibitlity which

**varies**slowlywith

**temperature**, making extrapolation of the high**temperature**results tricky ...### What people are saying - Write a review

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### Contents

LOMER Band theory and magnetism | 1 |

PHILLIPS Band theory of transition metals | 22 |

JACCARINO Studies of the hyperfine interaction in transi | 39 |

Copyright | |

19 other sections not shown

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### Common terms and phrases

alloys appearance approximation assume average band becomes bound boundary calculation charge complex computed condition conduction consider contribution correct correlation corresponding coupling curve defined density depends determined direction discussed effect electrons energy equation exchange existence expected expression fact factor Fermi Fermi level Fermi surface ferromagnetic field function given gives Hamiltonian host metal impurity atom increases integral interaction interesting lattice limit localized magnetic matrix elements means method moments normal Note observed obtained occur operator orbital perturbation phase Phys physical plane polarization poles positive possible potential present problem properties range relation replaced represent resonance scattering screening Sect shift shown similar simple single solution spin strong structure temperature theory tion transition metals usual wave wave functions write zero