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

### From inside the book

Results 1-3 of 77

Page 249

Two of them

magnetization of the host metal and the other to a small impurity moment . In this

case we have to calculate the energies

...

Two of them

**correspond**to the impurity moment parallel and antiparallel to themagnetization of the host metal and the other to a small impurity moment . In this

case we have to calculate the energies

**corresponding**to these three solutions in...

Page 288

This

( eq . ... Going now to a transitional metal

ok number ; the

This

**corresponds**to taking into account the non - d part y ' of the Bloch functions y( eq . ... Going now to a transitional metal

**corresponds**to a reduction in atomic 5ok number ; the

**corresponding**repulsion potential v acts more strongly on Fig .Page 436

The wave number

beyond g . ( 2m ) , the wave number Qm of the SDW state of lowest energy

decreases continuously below lm Vm = Qm ( g ) < Qm . Because « m < < 2kp for g

> g .

The wave number

**corresponding**to QM = Q , in Sect . 3°6 is qe . As g increasesbeyond g . ( 2m ) , the wave number Qm of the SDW state of lowest energy

decreases continuously below lm Vm = Qm ( g ) < Qm . Because « m < < 2kp for g

> g .

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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 | |

25 other sections not shown

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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