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

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Page 79

Then the final step in the problem is to determine ai : what radial

= Nilzer ) + a . Ii ( ver ) in the region between the muffin tin radius Rm and the

nearest other atom ( > Rs ) satisfies outgoing boundary conditions as r = 0 when

the ...

Then the final step in the problem is to determine ai : what radial

**wave**function fi= Nilzer ) + a . Ii ( ver ) in the region between the muffin tin radius Rm and the

nearest other atom ( > Rs ) satisfies outgoing boundary conditions as r = 0 when

the ...

Page 88

The second effect concerns unlike spins which stay apart from each other

because their

potential . Parallel spinsare similarly affected but , because of the exclusion hole

...

The second effect concerns unlike spins which stay apart from each other

because their

**wave**functions correlate to avoid the electron - electron Coulombpotential . Parallel spinsare similarly affected but , because of the exclusion hole

...

Page 406

However , MARSHALL [ 16 ] has used phenomenological arguments to develop

a spin -

, in turn , give rise to a T term in D . IZUYAMA and KUBO [ 17 ] , again using the ...

However , MARSHALL [ 16 ] has used phenomenological arguments to develop

a spin -

**wave**Hamiltonian which includes interactions between spinwaves which, in turn , give rise to a T term in D . IZUYAMA and KUBO [ 17 ] , again using 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 | |

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