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Magnetism and superconductivity in Ru(1-x)Sr2RECu(2+x)O(8-d) (RE=Gd, Eu) and RuSr2Gd(1-y)Ce(y)Cu2O8 compounds by Klamut, P. W.; Dabrowski, B.; Mini, S. M.; Kolesnik, S.; Maxwell, M.; Mais, J.; Shengelaya, A.; Khazanov, R.; Savic, I.; Keller, H.; Sulkowski, C.; Wlosewicz, D.; Matusiak, M.; Wisniewski, A.; Puzniak, R.; Fita, I. is a scholarly article available to read on EtoBox.

What is Magnetism and superconductivity in Ru(1-x)Sr2RECu(2+x)O(8-d) (RE=Gd, Eu) and RuSr2Gd(1-y)Ce(y)Cu2O8 compounds about?

We discuss the properties of new superconducting compositions of Ru(1-x)Sr2RECu(2+x)O(8-d) (RE=Gd, Eu) ruthenocuprates that were synthesized at 600 atm. of oxygen at 1080 C. By changing ratio between the Ru and Cu, the temperature of superconducting transition (Tc) raises up to Tc max=72 K for x=0.3, 0.4. The hole doping achieved along the series increases with Cu->Ru substitution. For x different than x=0, Tc can be subsequently tuned between Tc max and 0 K by changing oxygen content in the compounds. The magnetic characteristics of the RE=Gd and Eu based compounds are interpreted as indicative of constrained dimensionality of the superconducting phase. Muon spin rotation experiments reveal the presence of the magnetic transitions at low temperatures (Tm=14-2 K for x=0.1-0.4) that can originate in the response of Ru/Cu sublattices. RuSr2Gd(1-y)Ce(1-y)Cu2O8 (0<y<0.1) compounds show the simultaneous increase of TN and decrease of Tc with y. The effect should be explained by the electron doping that occurs with Ce->Gd substitution. Properties of these two series allow us to propose phase diagram for 1212-type ruthenocuprates that links their properties to the hole doping achieved in

Author

Klamut, P. W.; Dabrowski, B.; Mini, S. M.; Kolesnik, S.; Maxwell, M.; Mais, J.; Shengelaya, A.; Khazanov, R.; Savic, I.; Keller, H.; Sulkowski, C.; Wlosewicz, D.; Matusiak, M.; Wisniewski, A.; Puzniak, R.; Fita, I.

Published

2002

Language

EN