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

### From inside the book

Results 1-3 of 90

Page 5

Consider setting up the

The ground state of the atom is the configuration ( 48 ) + ( 3d ) “ , and ( 48 ) 2 ( 3d

) ; and ( 3d ) 5 lie not far away . We may well expect that the charge density round

...

Consider setting up the

**calculation**of the band structure of metallic vanadium .The ground state of the atom is the configuration ( 48 ) + ( 3d ) “ , and ( 48 ) 2 ( 3d

) ; and ( 3d ) 5 lie not far away . We may well expect that the charge density round

...

Page 52

In this paper we present a new method for

energy in a multiple - scattering system , which has the ... in principle the starting

formulas are exact , many approximations are necessary to do an actual

In this paper we present a new method for

**calculating**the density of states inenergy in a multiple - scattering system , which has the ... in principle the starting

formulas are exact , many approximations are necessary to do an actual

**calculation**.Page 53

In fact , it gives a valid result on integrating over any volume . To do the multiple

scattering

a single scatterer ; the potentials of no two scatterers are allowed to overlap .

In fact , it gives a valid result on integrating over any volume . To do the multiple

scattering

**calculation**, we divide the volume up into cells in each one of which isa single scatterer ; the potentials of no two scatterers are allowed to overlap .

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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