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Interactions aspherical Coulomb

If instead of the isotropic exchange interaction (A, S) = (0,1) we consider the aspherical Coulomb interaction (A, 2 ) = (2,0) we obtain fig. 17.15 instead. The negative sign for y indicates pair-enhancement instead of pair-breaking. Since this is a dynamical effect it vanishes for 5 = 0. The maximum effect occurs for 8 = lOTc. It resembles the one of additional Einstein oscillators put into the matrix. The quantity t, in the definition of y has to be replaced by to which is defined in a similar way as Ts (see eq. (17.66)) but now with Hac instead of He. ... [Pg.328]

In order to study the influence of conduction electrons we restrict ourselves to the aspherical Coulomb charge scattering A, S) = (2,0) which is described by the hamiltonian H c as given by eq. (17.44). Furthermore we consider again the simple case of cubic symmetry and specialize our considerations to a shear wave polarized in x-direction and propagating in z-direction. The interaction of the RE-ions via the conduction electrons is taken into account by extending the diagrammatic equations for the mode under consideration so that they are of the form shown in fig. 17.39. [Pg.359]


See other pages where Interactions aspherical Coulomb is mentioned: [Pg.235]    [Pg.238]    [Pg.239]    [Pg.256]    [Pg.271]    [Pg.315]    [Pg.326]    [Pg.381]    [Pg.382]    [Pg.42]   
See also in sourсe #XX -- [ Pg.315 ]




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