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

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Page 140

Also the Wronskian 0 / ( kr ) Øl - kr ) — 0 , ( k , r ) ' ( - kr ) , is a

the asymptotic form of 0 the

further requirement that u ( kr ) + ( 1 + 1 ) p ? we see that P : ( k ) = - ( 1 + 1 ) ...

Also the Wronskian 0 / ( kr ) Øl - kr ) — 0 , ( k , r ) ' ( - kr ) , is a

**constant**, and fromthe asymptotic form of 0 the

**constant**is seen to be 6 ) 2ik . From this and from thefurther requirement that u ( kr ) + ( 1 + 1 ) p ? we see that P : ( k ) = - ( 1 + 1 ) ...

Page 326

In principle it is possible to make neutron measurements at

transfers q , but in practice , for energies in this range , at the present state of

knowledge of neutron flux , etc . , it becomes more practical to measure the

inelastic ...

In principle it is possible to make neutron measurements at

**constant**momentumtransfers q , but in practice , for energies in this range , at the present state of

knowledge of neutron flux , etc . , it becomes more practical to measure the

inelastic ...

Page 400

Without going into the details of the calculation ( see reference [ 9 ] ) , one can

make the following comments : the number of electrons which are screened

around the two impurities is not

if we ...

Without going into the details of the calculation ( see reference [ 9 ] ) , one can

make the following comments : the number of electrons which are screened

around the two impurities is not

**constant**; it varies with R and even at**constant**Rif we ...

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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