E. V. Kuzmin1, *, S. G. Ovchinnikov2, **, I. O. Baklanov2, and E. G. Goryachev1
1 Krasnoyarsk State University, Krasnoyarsk, 660062 Russia
2 Kirenskii Institute of Physics, Siberian Division, Russian Academy of Sciences, Krasnoyarsk, 660036 Russia
*e-mail: evk@iph.krasn.ru
**e-mail: sgo@iph.krasn.ru
Received December 30, 1999
AbstractA microscopic tJI model with competing antiferromagnetic (J) and ferromagnetic (I) exchange
interactions is proposed for strongly correlated electrons in RuSr2GdCu2O8 . It is assumed that J
I for CuO2
layers and J
I for RuO2 layers. A superconducting solution of
symmetry was obtained for the CuO2
layers while competition between ferromagnetism and p-type triplet superconducting pairing is obtained for
RuO2 layers. It is shown that the RuO2 layers have a lower carrier concentration in the Hubbard subband formed
by coupled ((dxyp)
) orbitals compared with a bulk Sr2RuO4 crystal, which leads to stabilization of the fer-
romagnetic state in the RuO2 layer. © 2000 MAIK Nauka/Interperiodica.
Pleiades Publishing home page | journal home page | top
If you have any problems with this server, contact webmaster.