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

### From inside the book

Results 1-3 of 54

Page 129

An additional

products . ... Therefore each thermal average must be multiplied by a

( 28 + 1 ) , one such

An additional

**factor**is required to yield the same averages as would the real spinproducts . ... Therefore each thermal average must be multiplied by a

**factor**epa /( 28 + 1 ) , one such

**factor**for each impurity spin occurring in the average ...Page 185

An alternative recipe would have been to always adopt the integral for log R but

to multiply R by the Blaschke

does not change the equation for 8 " , and so any solution obtained from R by ...

An alternative recipe would have been to always adopt the integral for log R but

to multiply R by the Blaschke

**factor**... for T < Tc . Since this**factor**is unimodular itdoes not change the equation for 8 " , and so any solution obtained from R by ...

Page 327

Finally , to get the measured cross - section one must multiply [ 1 ] in a tight -

binding model , by the form

atomic wave functions ( 26 ) F ( g ) = fa•elg ( a ) | * expliq . x ] " This turns out to fall

...

Finally , to get the measured cross - section one must multiply [ 1 ] in a tight -

binding model , by the form

**factor**for the neutron plane waves interacting with theatomic wave functions ( 26 ) F ( g ) = fa•elg ( a ) | * expliq . x ] " This turns out to fall

...

### What people are saying - Write a review

We haven't found any reviews in the usual places.

### 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

### Other editions - View all

### 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