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

### From inside the book

Results 1-3 of 49

Page 41

3 ) to

the the value

of ...

3 ) to

**determine**the average value of W ( 9 ) 8 - . ... elements will enable us to**determine**the 0 . ... Keeping E , fixed at the Cu conduction bands as a function ofthe the value

**determined**by the neck position of the d bands ( preliminary resultsof ...

Page 43

3 ) can be evaluated from the eigenfunctions of Mueller ' s model Hamiltonian

provided that we

enters the sum rules at L and at X , and the values

% .

3 ) can be evaluated from the eigenfunctions of Mueller ' s model Hamiltonian

provided that we

**determine**the matrix element ( 3p ... The same matrix elemententers the sum rules at L and at X , and the values

**determined**agree to within 10% .

Page 432

The P - F boundary was

SAWADA [ 81 ] . The P - A boundary was

OVERHAUSER [ 69 ] by numerical solution of ( 86 ) . Note that

antiferromagnetism occurs for ...

The P - F boundary was

**determined**from ( 87 ) first derived by IWAMATO andSAWADA [ 81 ] . The P - A boundary was

**determined**by HAMANN andOVERHAUSER [ 69 ] by numerical solution of ( 86 ) . Note that

antiferromagnetism occurs for ...

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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