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

### From inside the book

Results 1-3 of 57

Page 117

If there is no interaction with the band electrons , one can immediately decide

whether or not the momentum is finite : it is finite , if the single particle energy of

the orbital is below the

If there is no interaction with the band electrons , one can immediately decide

whether or not the momentum is finite : it is finite , if the single particle energy of

the orbital is below the

**Fermi level**, but twice the single particle energy plus the ...Page 277

The perturbation diagram contributing to this in the scattering amplitude to lowest

order in J is a third - order diagram This contributes a part to the cross - section

which is asymmetric about the

The perturbation diagram contributing to this in the scattering amplitude to lowest

order in J is a third - order diagram This contributes a part to the cross - section

which is asymmetric about the

**Fermi level**, resulting from the small imaginary ...Page 395

In an old paper , Friedel ( see for example [ 1 ] ) explained the residual resitivity of

the transitional series in copper which depends only upon the phase shift at the

In an old paper , Friedel ( see for example [ 1 ] ) explained the residual resitivity of

the transitional series in copper which depends only upon the phase shift at the

**Fermi level**. Particularly striking is the fact that the resistivity per 1 % of ...### What people are saying - Write a review

We haven't found any reviews in the usual places.

### 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

### Other editions - View all

### 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