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

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Page 40

There is a difference between effective masses calculated in the one

theory and the effective masses associated with extremal cross sections of the

Fermi surface measured in dHvA or cyclotron resonance experiments [ 41 ] .

There is a difference between effective masses calculated in the one

**electron**theory and the effective masses associated with extremal cross sections of the

Fermi surface measured in dHvA or cyclotron resonance experiments [ 41 ] .

Page 105

An

adding one

An

**electron**hopping onto an atom can go into a variety of states since the ( n + 1 )**electron**system has many configurations several of which can be reached byadding one

**electron**to the n -**electron**configuration . In the atomic limit many ...Page 193

At the present time we are therefore unable to settle the interesting question of

whether there is a partial or complete compensation of the bare Curie constant by

the resonant

...

At the present time we are therefore unable to settle the interesting question of

whether there is a partial or complete compensation of the bare Curie constant by

the resonant

**electron**. A similar problem faces the evaluation of the specific heat...

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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