Proceedings of the International School of Physics "Enrico Fermi.", Volume 37N. Zanichelli, 1967 - Nuclear physics |
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Page 7
For this metal there are four electrons outside the rare - gas shell , and some
occupancy is expected in 8 , d and f - like levels . The calculations assumed the -
0 . 4 E ( Ryd ) - 0 . 8 MA YA 4 , 11 2 . 0 - 16 x = 1 . 5 X = 1 . 0 x = 0 . 5 - 1 . 6 ' 1x32 .
For this metal there are four electrons outside the rare - gas shell , and some
occupancy is expected in 8 , d and f - like levels . The calculations assumed the -
0 . 4 E ( Ryd ) - 0 . 8 MA YA 4 , 11 2 . 0 - 16 x = 1 . 5 X = 1 . 0 x = 0 . 5 - 1 . 6 ' 1x32 .
Page 217
We have assumed here , for brevity , that the impurity potential is localized within
the impurity atom cell , i . e . , only the nonvanishing matrix element of Hi is
assumed to be the diagonal one for the impurity atom orbital . The Coulomb and
...
We have assumed here , for brevity , that the impurity potential is localized within
the impurity atom cell , i . e . , only the nonvanishing matrix element of Hi is
assumed to be the diagonal one for the impurity atom orbital . The Coulomb and
...
Page 379
zation is of any significance . We must therefore assume that an
antiferromagnetic polarization of the s conduction electron appears on atoms
adjacent to a given magnetic d - atom since no moment is intrinsic to those
impurity atoms . It is also ...
zation is of any significance . We must therefore assume that an
antiferromagnetic polarization of the s conduction electron appears on atoms
adjacent to a given magnetic d - atom since no moment is intrinsic to those
impurity atoms . It is also ...
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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 | |
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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