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

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Page 118

From the success of this approximation in the treatment of dilute systems these

authors inferred that if conditions were such that the extra orbital was almost

have ...

From the success of this approximation in the treatment of dilute systems these

authors inferred that if conditions were such that the extra orbital was almost

**completely**empty , or almost**completely**filled then the correlation energy wouldhave ...

Page 291

Ferromagnetism : It can also happen that one half d band be - a ) weak ; b )

strong . comes

86 ) . We shall then talk of a strong ferromagnetism [ 4 ] . The condition for strong

...

Ferromagnetism : It can also happen that one half d band be - a ) weak ; b )

strong . comes

**completely**full ( or empty ) when ñŪ , is still larger than unity ( Fig .86 ) . We shall then talk of a strong ferromagnetism [ 4 ] . The condition for strong

...

Page 450

The merest glimpse at the phase diagrams of the liquid simple metals shows that

the alkali metals are unique and

pertinent features of the phase diagrams of the liquid simple metals can be ...

The merest glimpse at the phase diagrams of the liquid simple metals shows that

the alkali metals are unique and

**completely**anomalous in their behavior . Thepertinent features of the phase diagrams of the liquid simple metals can be ...

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### Contents

LOMER Band theory and magnetism | 1 |

PHILLIPS Band theory of transition metals | 22 |

JACCARINO Studies of the hyperfine interaction in transi | 39 |

Copyright | |

19 other sections not shown

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### Common terms and phrases

alloys appearance approximation assume average band becomes bound boundary calculation charge complex computed condition conduction consider contribution correct correlation corresponding coupling curve defined density depends determined direction discussed effect electrons energy equation exchange existence expected expression fact factor Fermi Fermi level Fermi surface ferromagnetic field function given gives Hamiltonian host metal impurity atom increases integral interaction interesting lattice limit localized magnetic matrix elements means method moments normal Note observed obtained occur operator orbital perturbation phase Phys physical plane polarization poles positive possible potential present problem properties range relation replaced represent resonance scattering screening Sect shift shown similar simple single solution spin strong structure temperature theory tion transition metals usual wave wave functions write zero