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

### From inside the book

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Page 33

This efrepulsive fect can be described by an off - diagonal 2V ( AI ) orthogonality

splitting matrix element , direct 2V ( Cu ) hybridization ... Note that k = al / 4 the

hybridizing form factor g ( k ) is assumed to be isotropic ; it is

This efrepulsive fect can be described by an off - diagonal 2V ( AI ) orthogonality

splitting matrix element , direct 2V ( Cu ) hybridization ... Note that k = al / 4 the

hybridizing form factor g ( k ) is assumed to be isotropic ; it is

**shown in Fig**. 1 .Page 38

The bands are

are filled , and the Fermi energy falls just above the conduction band edge Lg .

As a consequence the Fermi surface consists in each Brillouin zone of a ...

The bands are

**shown**along certain symmetry directions in**Fig**. 5 . The d bandsare filled , and the Fermi energy falls just above the conduction band edge Lg .

As a consequence the Fermi surface consists in each Brillouin zone of a ...

Page 42

The preliminary result is

correspond to AE < 0 . ... graphical methods can lead to errors in placing the d

bands relative to the conduction bands of more than 1 eV . From Fig . 8 and eq . (

4 .

The preliminary result is

**shown in Fig**. ... 33 , which from the Figure is seen tocorrespond to AE < 0 . ... graphical methods can lead to errors in placing the d

bands relative to the conduction bands of more than 1 eV . From Fig . 8 and eq . (

4 .

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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