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

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Page 39

074 rely on Fermi surface data to fix the position of the d bands and

bands . 1 . 03 . In the nonmagnetic metals Pd and Pt the preliminary evidence [

34 , 39 ] indicates that apart from larger spin - orbit splittings of d levels the

energy ...

074 rely on Fermi surface data to fix the position of the d bands and

**conduction**bands . 1 . 03 . In the nonmagnetic metals Pd and Pt the preliminary evidence [

34 , 39 ] indicates that apart from larger spin - orbit splittings of d levels the

energy ...

Page 226

The total change in the number of

admixture with the impurity atom is given by EF ( 1 . 1 ) ene = fåe og male ) = –

452 ) im jästoleycode ) , where second ( s ) has already been calculated in ( 2 .

The total change in the number of

**conduction**electrons due to the covalentadmixture with the impurity atom is given by EF ( 1 . 1 ) ene = fåe og male ) = –

452 ) im jästoleycode ) , where second ( s ) has already been calculated in ( 2 .

Page 261

22 ) F ( x ) = x cos x — sin x x 1 and Q , is the

Similarly for o ( r ) with f→ - f . Thus the total charge density exto does not oscillate

in this model ( we neglect effects due to a spin - independent potential ) while the

total ...

22 ) F ( x ) = x cos x — sin x x 1 and Q , is the

**conduction**electron density .Similarly for o ( r ) with f→ - f . Thus the total charge density exto does not oscillate

in this model ( we neglect effects due to a spin - independent potential ) while the

total ...

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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