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

### From inside the book

Results 1-3 of 45

Page 286

Such peaks are indeed a feature of the n ( E )

in the tight - binding approximation [ 2 ] ... In the BCC structure , a strong structure

( schematic ) . minimum of the computed n ( E ) divides the

Such peaks are indeed a feature of the n ( E )

**curves**computed for liquid crystalsin the tight - binding approximation [ 2 ] ... In the BCC structure , a strong structure

( schematic ) . minimum of the computed n ( E ) divides the

**curve**in two parts ...Page 301

behaviour of the Slater - Pauling

average moment in ferromagnetic alloys ( Fig . 1 ) . a ) In Ni or Co ( Fig . 9a , b ) ,

where one half d - band ( with spin up ) is full , the shifting of the bands produced

...

behaviour of the Slater - Pauling

**curve**ū ( N ) reported earlier , which gives theaverage moment in ferromagnetic alloys ( Fig . 1 ) . a ) In Ni or Co ( Fig . 9a , b ) ,

where one half d - band ( with spin up ) is full , the shifting of the bands produced

...

Page 448

As one starts out from high densities , V , remains relatively unimportant and AE

decreases relative to V . Thus there ultimately must come a density at which a

mechanical instability would set in , a horizontal point of a p - V

As one starts out from high densities , V , remains relatively unimportant and AE

decreases relative to V . Thus there ultimately must come a density at which a

mechanical instability would set in , a horizontal point of a p - V

**curve**. As one ...### 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