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

### From inside the book

Results 1-3 of 41

Page 237

6 ,

contributions are not subtracted from the susceptibility data . This correction ,

however , does not seem to be very important . A possibly more important

correction ...

6 ,

**respectively**. In these estimations diamagnetic and orbital paramagneticcontributions are not subtracted from the susceptibility data . This correction ,

however , does not seem to be very important . A possibly more important

correction ...

Page 240

This result may be interpreted as follows : The virtual impurity states with the

width 4 for the atoms 1 and 2 are located at Eo and E , ,

is no interaction between them . When the covalent admixture is introduced

between ...

This result may be interpreted as follows : The virtual impurity states with the

width 4 for the atoms 1 and 2 are located at Eo and E , ,

**respectively**when thereis no interaction between them . When the covalent admixture is introduced

between ...

Page 338

Let r , and r . be the position vectors for the elements of the charge distributions q

, and 9 . in the nucleus and electronic charge cloud

of the nucleus as the origin . Then the electrostatic interaction energy is ( 1 .

Let r , and r . be the position vectors for the elements of the charge distributions q

, and 9 . in the nucleus and electronic charge cloud

**respectively**with the centroidof the nucleus as the origin . Then the electrostatic interaction energy is ( 1 .

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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