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

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Page 58

Jy is in fact the function

0 and is therefore expressible outside the muffin tin as : ( 2 . 11 ) Julęr ) = cos 8 ,

( xr ) — sin dinzlęr ) pe > Rm , fi is

Jy is in fact the function

**defined**earlier which obeys the boundary condition at p =0 and is therefore expressible outside the muffin tin as : ( 2 . 11 ) Julęr ) = cos 8 ,

( xr ) — sin dinzlęr ) pe > Rm , fi is

**defined**by two requirements : first , that its ...Page 221

... 6 ) , where ner , Neo and noo are

energy ε in the localized e , and tz , orbitals , respectively , in the unperturbed

system .

... 6 ) , where ner , Neo and noo are

**defined**by ( 2 . 17 ) . nele ) and no ( s )**defined**by ( 3 . 17 ) represent the probability densities to find the electrons withenergy ε in the localized e , and tz , orbitals , respectively , in the unperturbed

system .

Page 251

Observed temperature dependence of the internal field at 55 Mn in Fe [ 30 ]

suggests the possible existence of a fairly well

couples rather weakly to the Fe matrix [ 31 ] . This weak coupling seems to be

understood ...

Observed temperature dependence of the internal field at 55 Mn in Fe [ 30 ]

suggests the possible existence of a fairly well

**defined**Mn moment whichcouples rather weakly to the Fe matrix [ 31 ] . This weak coupling seems to be

understood ...

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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