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

### From inside the book

Results 1-3 of 75

Page vii

Effect of exchange

of the spin polarization . . . . . . 234 4 ' 5 . Giant moments in palladium and

platinum alloys . . . 5 .

1 .

Effect of exchange

**interaction**in the host metal . . . 230 4 ' 4 . Spatial distributionof the spin polarization . . . . . . 234 4 ' 5 . Giant moments in palladium and

platinum alloys . . . 5 .

**Interaction**between two impurity atoms . . . . . . . . . . . 238 5 '1 .

Page 46

Because electrostatic

Coulomb

range ) , the effect of using a pseudoWannier basis is to reduce the strength ...

Because electrostatic

**interactions**in the metal are screened , so that theCoulomb

**interaction**is replaced by an**interaction**of the Yukawa type ( short -range ) , the effect of using a pseudoWannier basis is to reduce the strength ...

Page 431

Clearly , it would be extremely tedius to solve ( 78 ) for A , construct the total

energy U from ( 82 ) , and then minimize U as a function of Q for a general

the linear ...

Clearly , it would be extremely tedius to solve ( 78 ) for A , construct the total

energy U from ( 82 ) , and then minimize U as a function of Q for a general

**interaction**. Accordingly , we shall find a simple , parametrized form of ve , solvethe linear ...

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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