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

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Page 336

where Li and S , are the orbital and spin operators of the individual nucleons , the

aforementioned restrictions are : 1 )

with n an integer 0 , 1 , . . . ; i . e . have odd half - integral values of I . 2 )

where Li and S , are the orbital and spin operators of the individual nucleons , the

aforementioned restrictions are : 1 )

**Nuclei**with A an odd number have I = ( n + } )with n an integer 0 , 1 , . . . ; i . e . have odd half - integral values of I . 2 )

**Nuclei**...Page 343

We only have established that the

extent , electrostatic probe of matter . ... Consider an ensemble of noninteracting

, ...

We only have established that the

**nucleus**can be a magnetic and , to a certainextent , electrostatic probe of matter . ... Consider an ensemble of noninteracting

**nuclei**N all with I = } , for simplicity , and all in the same external magnetic field H, ...

Page 397

The frequency displacements due to 1 ) and 2 ) are so large compared with the

line width that a number n of

experiments . The intensity I of the line behaves as log - n log ( 1 - 0 ) – – nc , 1 ...

The frequency displacements due to 1 ) and 2 ) are so large compared with the

line width that a number n of

**nuclei**around each Mn are not observed in NMRexperiments . The intensity I of the line behaves as log - n log ( 1 - 0 ) – – nc , 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