Proceedings of the International School of Physics "Enrico Fermi.", Volume 37N. Zanichelli, 1967 - Nuclear physics |
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Results 1-3 of 41
Page 237
6 , respectively . In these estimations diamagnetic and orbital paramagnetic
contributions are not subtracted from the susceptibility data . This correction ,
however , does not seem to be very important . A possibly more important
correction ...
6 , respectively . In these estimations diamagnetic and orbital paramagnetic
contributions are not subtracted from the susceptibility data . This correction ,
however , does not seem to be very important . A possibly more important
correction ...
Page 240
This result may be interpreted as follows : The virtual impurity states with the
width 4 for the atoms 1 and 2 are located at Eo and E , , respectively when there
is no interaction between them . When the covalent admixture is introduced
between ...
This result may be interpreted as follows : The virtual impurity states with the
width 4 for the atoms 1 and 2 are located at Eo and E , , respectively when there
is no interaction between them . When the covalent admixture is introduced
between ...
Page 338
Let r , and r . be the position vectors for the elements of the charge distributions q
, and 9 . in the nucleus and electronic charge cloud respectively with the centroid
of the nucleus as the origin . Then the electrostatic interaction energy is ( 1 .
Let r , and r . be the position vectors for the elements of the charge distributions q
, and 9 . in the nucleus and electronic charge cloud respectively with the centroid
of the nucleus as the origin . Then the electrostatic interaction energy is ( 1 .
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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