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

### From inside the book

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Page 53

Outside the cell we ask merely « how does the spherical wave of angular

back into that cell ? » ( i . e . , we put on outgoing boundary conditions and ask for

the ...

Outside the cell we ask merely « how does the spherical wave of angular

**momentum**l emanating from cell į propagate , and in particular how is it reflectedback into that cell ? » ( i . e . , we put on outgoing boundary conditions and ask for

the ...

Page 197

... ex = ko and Wxx ( 8 ) the probability of passing from side 1 at energy a and

dependence on

balance .

... ex = ko and Wxx ( 8 ) the probability of passing from side 1 at energy a and

**momentum**k to side 2 at**momentum**k ' . As already stated we neglect thedependence on

**momentum**subscripts . Further , W12 = W21 = W by detailedbalance .

Page 326

In principle it is possible to make neutron measurements at constant

transfers q , but in practice , for energies in this range , at the present state of

knowledge of neutron flux , etc . , it becomes more practical to measure the

inelastic ...

In principle it is possible to make neutron measurements at constant

**momentum**transfers q , but in practice , for energies in this range , at the present state of

knowledge of neutron flux , etc . , it becomes more practical to measure the

inelastic ...

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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