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

### From inside the book

Results 1-3 of 4

Page 27

Both these drawbacks can be overcome by transforming to

The

orthogonalized plane waves [ 17 ] . These have the form ( 2 . 1 ) Yn = N . [ 4x -

Eber ] ...

Both these drawbacks can be overcome by transforming to

**natural**basis states .The

**natural**basis functions for the s - p conduction band are Herring ' sorthogonalized plane waves [ 17 ] . These have the form ( 2 . 1 ) Yn = N . [ 4x -

Eber ] ...

Page 28

In a crystal , of course , the important values of q are those equal to the first two or

three reciprocal lattice vectors Kn . The

course , the atomic orbitals discussed in the preceding Section . By a swindle ...

In a crystal , of course , the important values of q are those equal to the first two or

three reciprocal lattice vectors Kn . The

**natural**basis states for the d states are , ofcourse , the atomic orbitals discussed in the preceding Section . By a swindle ...

Page 377

The reasons for this are largely experimental : a ) The 57Fe ME has the requisite

resolution only when the internal fields exceed the

kOe , b ) There is a large enhancement of the driving radio - frequency field in an

...

The reasons for this are largely experimental : a ) The 57Fe ME has the requisite

resolution only when the internal fields exceed the

**natural**line - width SH ~ 10kOe , b ) There is a large enhancement of the driving radio - frequency field in an

...

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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