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

### From inside the book

Results 1-3 of 18

Page 103

... n - , W respectively . Because of their residues they contain 1 - n _ , and n _ o

states . Thus the picture is of two bands narrowed but not changed in

) .

... n - , W respectively . Because of their residues they contain 1 - n _ , and n _ o

states . Thus the picture is of two bands narrowed but not changed in

**shape**(**shape**changes are due to q dependence of the numerator and occur to order 1 / I) .

Page 366

Since wo , the nuclear resonance frequency , is very small we may replace x ( 0 ,

0 ) x 19 , 0 ) 9 / 2K4 Fig . 14 . x . ( q , w ) by xólq , 0 ) . Consider an idealized

polarization ...

Since wo , the nuclear resonance frequency , is very small we may replace x ( 0 ,

0 ) x 19 , 0 ) 9 / 2K4 Fig . 14 . x . ( q , w ) by xólq , 0 ) . Consider an idealized

**shape**for xó ( 9 , 0 ) as shown above . Then for spin - dependent d corepolarization ...

Page 426

We note , however , that the observed line

agree with their calculated line

contamination of the K surface may possibly have been responsible for the

observed ...

We note , however , that the observed line

**shape**of the helicon edge in K did notagree with their calculated line

**shape**, which implies that imperfection orcontamination of the K surface may possibly have been responsible for the

observed ...

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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