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

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Page 133

we see by

+ 0 . ) , exp [ 1957 – 10 . ) - - * * explilaj , # + ( 22 + 13a / 29 = . 0 , exp [ - * + 10 . )

and From the first of these equations we have and so , from the second a : ( k ) ...

we see by

**comparison**of ( 9 ) with the asymptotic solution that ys = 0 , sin ( kor – "+ 0 . ) , exp [ 1957 – 10 . ) - - * * explilaj , # + ( 22 + 13a / 29 = . 0 , exp [ - * + 10 . )

and From the first of these equations we have and so , from the second a : ( k ) ...

Page 368

Care has to be exerted to observe only the resonance in the domains if a simple

found that 1 / T , ~ T , indicating that the primary source of relaxation is the ...

Care has to be exerted to observe only the resonance in the domains if a simple

**comparison**between theory and experiment is to be made . In Fe , Co and Ni it isfound that 1 / T , ~ T , indicating that the primary source of relaxation is the ...

Page 397

The

factor of the order of two . The conclusion does not disagree with the first NMR

experiments on Cu Mn which were done by KNIGHT et al : they concluded that

no ...

The

**comparison**is nearly excellent if the magnetic contribution is reduced by afactor of the order of two . The conclusion does not disagree with the first NMR

experiments on Cu Mn which were done by KNIGHT et al : they concluded that

no ...

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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