Proceedings of the International School of Physics "Enrico Fermi.", Volume 37N. Zanichelli, 1967 - Nuclear physics |
From inside the book
Results 1-3 of 56
Page 275
This term only gives a nonzero contribution because the spin operators 8 - , 8 +
do not commute . ( 2 . 8 ) is the logarithmically divergent term found by Kondo . It
gives rise to a cross - section which either increases ( J antiferromagnetic ) or ...
This term only gives a nonzero contribution because the spin operators 8 - , 8 +
do not commute . ( 2 . 8 ) is the logarithmically divergent term found by Kondo . It
gives rise to a cross - section which either increases ( J antiferromagnetic ) or ...
Page 354
K , : first it should be pointed out that the spin - dipolar interaction produces no
contribution to d - spin Knight shift . More precisely , in the absence of spin - orbit
coupling and in cubic symmetry the diagonal elements , ( 3 . 16 ) s Km , kơ 3r ( s .
r ) ...
K , : first it should be pointed out that the spin - dipolar interaction produces no
contribution to d - spin Knight shift . More precisely , in the absence of spin - orbit
coupling and in cubic symmetry the diagonal elements , ( 3 . 16 ) s Km , kơ 3r ( s .
r ) ...
Page 368
( Direct magnon processes , which would yield a 1 / T , ~ T make no significant
contribution to 1 / T , because of the scarcity of magnons with E = hwn ) . There is
also a spin wave contribution to i / T , that is proportional to T which arises from
the ...
( Direct magnon processes , which would yield a 1 / T , ~ T make no significant
contribution to 1 / T , because of the scarcity of magnons with E = hwn ) . There is
also a spin wave contribution to i / T , that is proportional to T which arises from
the ...
What people are saying - Write a review
We haven't found any reviews in the usual places.
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
Other editions - View all
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