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Superconductivity suppression of Ba0.5K0.5Fe2−2xM2xAs2 single crystals by substitution of transition metal (M = Mn, Ru, Co, Ni, Cu, and Zn)

J. Li, Y. F. Guo, S. B. Zhang, J. Yuan, Y. Tsujimoto, X. Wang, C. I. Sathish, Y. Sun, S. Yu, W. Yi, K. Yamaura, E. Takayama-Muromachiu, Y. Shirako, M. Akaogi, H. Kontani

DOI 10.1103/PhysRevB.85.214509 · Physical Review B

T1

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Abstract

We investigated the doping effects of magnetic and nonmagnetic impurities in single-crystalline p-type Ba0.5K0.5Fe2−2xM2xAs2 (M = Mn, Ru, Co, Ni, Cu, and Zn) superconductors. The superconductivity is maintained robustly with the impurity Ru, and weakly with the impurities Mn, Co, Ni, Cu, and Zn. However, the present Tc suppression rate of both magnetic and nonmagnetic impurities remains much lower than what was expected for the s±-wave model. The temperature dependence of resistivity data shows an obvious low-T upturn for the crystals doped with high levels of impurity, which is due to the occurrence of localization. Thus, the relatively weak Tc suppression effect from Mn, Co, Ni, Cu, and Zn is considered to be a result of localization rather than the pair-breaking effect in the s±-wave model.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
Ba0.5K0.5Fe2As2

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37.78Pressure not reportedunknown
Ba0.5K0.5Fe1.922Mn0.078As2

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9.53Pressure not reportedunknown
Ba0.5K0.5Fe1.936Ru0.064As2

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37.14Pressure not reportedunknown
Ba0.5K0.5Fe1.896Co0.104As2

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30.31Pressure not reportedunknown
Ba0.5K0.5Fe1.922Ni0.078As2

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Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

26.75Pressure not reportedunknown
Ba0.5K0.5Fe1.912Cu0.088As2

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Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

22.29Pressure not reportedunknown
Ba0.5K0.5Fe1.92Zn0.08As2

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30.15Pressure not reportedunknown

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