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

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Page 30

16 ) sin 12 = - 12 ( Kr ) U2y ( r ) rdr , where y is an outgoing wave related to the

projection qm of the d tight - binding state m ) on the d atomic state which has ma

, = ( L quantized along k ) . Near the

16 ) sin 12 = - 12 ( Kr ) U2y ( r ) rdr , where y is an outgoing wave related to the

projection qm of the d tight - binding state m ) on the d atomic state which has ma

, = ( L quantized along k ) . Near the

**resonance**energy Em , y assumes the form ...Page 31

22 ) – ( E - E ) KO Far from

. 19 ) , ( 2 . 21 ) and ( 2 . 22 ) to obtain the interpolation formula [ 18 ] 11 m d3y -

liąV 12 41 ( 2 . 23 ) - tg n2 = E - ES - 1 7 - ( E – EW ) K12 . E This expression for ...

22 ) – ( E - E ) KO Far from

**resonance**tg na — sin ng so that we may combine ( 2. 19 ) , ( 2 . 21 ) and ( 2 . 22 ) to obtain the interpolation formula [ 18 ] 11 m d3y -

liąV 12 41 ( 2 . 23 ) - tg n2 = E - ES - 1 7 - ( E – EW ) K12 . E This expression for ...

Page 199

Evidently we always get a

ferromagnetic ( < 0 ) or antiferromagnetic ( > 0 ) . To obtain a qualitative notion of

the result , suppose that g ( 1 ) = 0 , and let g ( 2 ) be antiferromagnetic , so the ...

Evidently we always get a

**resonance**, in 1 - 2 or 1 + 2 according as g « 2 ) isferromagnetic ( < 0 ) or antiferromagnetic ( > 0 ) . To obtain a qualitative notion of

the result , suppose that g ( 1 ) = 0 , and let g ( 2 ) be antiferromagnetic , so the ...

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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 | |

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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