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Superconductivity at 41 K and Its Competition with Spin-Density-Wave Instability in Layered CeO1−xFxFeAs

G. F. Chen, Z. Li, D. Wu, G. Li, W. Z. Hu, J. Dong, P. Zheng, J. L. Luo, N. L. Wang

DOI 10.1103/PhysRevLett.100.247002 · Physical Review Letters

T1

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Abstract

A series of layered CeO1−xFxFeAs compounds with x=0 to 0.20 are synthesized by the solid state reaction method. Similar to the LaOFeAs, the pure CeOFeAs shows a strong resistivity anomaly near 145 K, which was ascribed to the spin-density-wave instability. F doping suppresses this instability and leads to the superconducting ground state. Most surprisingly, the superconducting transition temperature could reach as high as 41 K. Such a high Tc strongly challenges the classic BCS theory based on the electron-phonon interaction. The closeness of the superconducting phase to the spin-density-wave instability suggests that the magnetic fluctuation plays a key role in the superconducting pairing mechanism. The study also reveals that the Ce 4f electrons form local moments and are ordered antiferromagnetically below 4 K, which could coexist with superconductivity.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
CeO1-xFxFeAs

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41Pressure not reportedonset
CeO1-xFxFeAs

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41Pressure not reportedonset
CeO0.84F0.16FeAs

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41Pressure not reportedonset
LaO1-xFxFeAs

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26Pressure not reportedunknown
CeRu2

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6.1Pressure not reportedunknown

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