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

### From inside the book

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Page 186

If evaluated in accordance with the former order , the solution varies smoothly as

J varies from positive to negative values ( a slight increase in conductivity seems

to

If evaluated in accordance with the former order , the solution varies smoothly as

J varies from positive to negative values ( a slight increase in conductivity seems

to

**occur**at low temperatures if J < 0 ( ferromagnetic in the present convention ) ) ...Page 432

7 ferromagnetic and P - A for paramagneticantiferromagnetic for that Q for which

instability first

by IWAMATO and SAWADA [ 81 ] . The P - A boundary was determined by ...

7 ferromagnetic and P - A for paramagneticantiferromagnetic for that Q for which

instability first

**occurs**. The P - F boundary was determined from ( 87 ) first derivedby IWAMATO and SAWADA [ 81 ] . The P - A boundary was determined by ...

Page 447

The fact that the gaseous phase

phase

consequence of the long - range repulsive nature of the electronelectron

interactions and ...

The fact that the gaseous phase

**occurs**at high densities and the crystallinephase

**occurs**at low densities , just the reverse of what ordinarily**occurs**, is aconsequence of the long - range repulsive nature of the electronelectron

interactions and ...

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### Contents

LOMER Band theory and magnetism | 1 |

JACCARINO Studies of the hyperfine interaction in transi | 39 |

P W ANDERSON and W L MCMILLAN Multiplescattering | 50 |

Copyright | |

25 other sections not shown

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### Common terms and phrases

alloys amplitude analytic Anderson approximation assume average band becomes Born bound calculation complex computed condition conduction consider contribution correct correlation corresponding coupling curve defined density depends determined discussed effect electrons energy equation exchange expected expression fact factor Fermi Fermi level ferromagnetic field function given gives Hamiltonian host metal impurity atom included integral interaction interesting lattice limit localized magnetic matrix element means metals method moments momentum normal obtained occur operator orbital particle perturbation Phys physical plane polarization poles positive possible potential present problem properties range relation replaced represent resonance scattering screening Sect seems shift shown similar simple solution spin structure surface temperature theory tion transition metals usual wave wave functions write written zero