Decoupled CuO2 and RuO2 layers in superconducting and magnetically ordered RuSr2GdCu2O8
M. Požek, A. Dulčić, D. Paar, A. Hamzić, M. Basletić, E. Tafra, G. V. M. Williams, S. Krämer
DOI 10.1103/PhysRevB.65.174514 · Physical Review B
Active bibliographic source — not scientific approval
Bibliographic access preserves source history; it does not approve extracted materials or validate reported claims. Review warnings on each occurrence separately.
Abstract
Comprehensive measurements of dc and ac susceptibility, dc resistance, magnetoresistance, Hall resistivity, and microwave absorption and dispersion in fields up to 8 T have been carried out on RuSr2GdCu2O8 with the aim to establish the properties of RuO2 and CuO2 planes. At ∼130 K, where the magnetic order develops in the RuO2 planes, one observes a change in the slope of dc resistance, change in the sign of magnetoresistance, and the appearance of an extraordinary Hall effect. These features indicate that the RuO2 planes are conducting. A detailed analysis of the ac susceptibility and microwave data on both ceramic and powder samples show that the penetration depth remains frequency dependent and larger than the London penetration depth even at low temperatures. We conclude that the conductivity in the RuO2 planes remains normal even when superconducting order is developed in the CuO2 planes below ∼45 K. Thus, experimental evidence is provided in support of theoretical models which base the coexistence of superconductivity and magnetic order on decoupled CuO2 and RuO2 planes.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| RuSr2GdCu2O8 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 45 | Pressure not reported | onset |
| RuSr2GdCu2O8 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 47 | Pressure not reported | onset |
| RuSr2GdCu2O8 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 35 | Pressure not reported | onset |
| Sr2RuO4 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
Similar papers
Antiferromagnetic ordering of Ru and Gd in superconducting RuSr2GdCu2O8
similarity 0.98J. W. Lynn et al.
Source status unknown — claims are unverified
Magnetic and electronic structures of superconducting RuSr2GdCu2O8
similarity 0.97K. Nakamura et al.
Source status unknown — claims are unverified
Decoupling of superconducting layers in the magnetic superconductor RuSr2GdCu2O8
similarity 0.97Manuel Houzet et al.
Source status unknown — claims are unverified
Superconductivity in Uniquely Strained RuO2 Films
similarity 0.97Masaki Uchida et al.
Source status unknown — claims are unverified
Towards universal magnetization curves in the superconducting state of RuSr2GdCu2O8
similarity 0.96Thomas P. Papageorgiou et al.
Source status unknown — claims are unverified
Ferromagnetic correlations and mixed Ru valence in the magnetic superconductor RuSr2(Eu,Gd)Cu2O8
similarity 0.96A. Butera et al.
Source status unknown — claims are unverified