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

### From inside the book

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Page 91

cost of changing two 3do

figures , depending on whether the energy cost is required for the ground state

cost of changing two 3do

**configurations**into a 3d10 and a 3d8 . ... This gives twofigures , depending on whether the energy cost is required for the ground state

**configuration**or whether an average is taken over possible**configurations**.Page 105

An electron hopping onto an atom can go into a variety of states since the ( n + 1 )

electron system has many

adding one electron to the n - electron

An electron hopping onto an atom can go into a variety of states since the ( n + 1 )

electron system has many

**configurations**several of which can be reached byadding one electron to the n - electron

**configuration**. In the atomic limit many ...Page 342

to find in the same 3d " 481

electrons ; H , = ( 893 ) 9B | Y ( 0 ) | The latter quantities were calculated TABLE I .

| Sc i Ti V Cr Mn Fe Co Ni Cu ; H , ( in 106 Oe ) ' 0 . 15 / 0 . 21 | H , ( in 106 Oe ) ...

to find in the same 3d " 481

**configuration**if there were no contribution from the d -electrons ; H , = ( 893 ) 9B | Y ( 0 ) | The latter quantities were calculated TABLE I .

| Sc i Ti V Cr Mn Fe Co Ni Cu ; H , ( in 106 Oe ) ' 0 . 15 / 0 . 21 | H , ( in 106 Oe ) ...

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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