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

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Page 121

absolute zero and with impurity spin } a singlet

antiferromagnetic coupling . This

of diagonalizing the Hamiltonian within the restricted manifold of states obtained

by ...

absolute zero and with impurity spin } a singlet

**bound**state is formed forantiferromagnetic coupling . This

**bound**state is obtained by the obvious methodof diagonalizing the Hamiltonian within the restricted manifold of states obtained

by ...

Page 149

It is also easily seen from the form of T , that a

1 leads to a T , that is a polynomial in v with highest power v ? For an 8 - wave

It is also easily seen from the form of T , that a

**bound**state with quantum number1 leads to a T , that is a polynomial in v with highest power v ? For an 8 - wave

**bound**state the subtraction ( 336 ) is appropriate , for 1 > 0 more elaborate ...Page 311

The

but lumped together in what one can call a virtual

to the presence of the broad s - band with which the d - levels will resonate , by a

...

The

**bound**states pictured in Fig . 1 are not split in two definite e , and t2 , states ,but lumped together in what one can call a virtual

**bound**level . This effect is dueto the presence of the broad s - band with which the d - levels will resonate , by a

...

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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