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

### From inside the book

Results 1-3 of 87

Page 31

Again we transform by ( 2.6 ) to rewrite the second term of ( 2.21 ) as ( 2.22 ) – ( E- E'Y ) KOM Far from resonance tg na — sin n . so that we may combine ( 2.19 ) , ( 2.21 ) and ( 2.22 ) to

Again we transform by ( 2.6 ) to rewrite the second term of ( 2.21 ) as ( 2.22 ) – ( E- E'Y ) KOM Far from resonance tg na — sin n . so that we may combine ( 2.19 ) , ( 2.21 ) and ( 2.22 ) to

**obtain**the interpolation formula [ 18 ] d3y ...Page 37

Direct information concerning the electronic structures of these metals can be

Direct information concerning the electronic structures of these metals can be

**obtained**from Fermi surface studies . In the case of magnetic metals such as Ni , we may hope to**obtain**from differences in 1 and Fermi surfaces estimates of ...Page 302

This charge 20 + 8zo is

This charge 20 + 8zo is

**obtained**by summing the electronic density no ( E ) over the occupied energies . To first order in V , eq . ( II.20 ) gives for the change in electronic charge on the impurity cell : Ey ...### 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