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Spin Ordering in LaFeAsO and Its Suppression in Superconductor LaFeAsO<sub>0.89</sub>F<sub>0.11</sub> Probed by Mössbauer Spectroscopy

Shinji KitaoCREST, Japan Science and Technology Agency, Kawaguchi, Saitama 332-0012Yasuhiro KobayashiCREST, Japan Science and Technology Agency, Kawaguchi, Saitama 332-0012Satoshi HigashitaniguchiCREST, Japan Science and Technology Agency, Kawaguchi, Saitama 332-0012Makina SaitoCREST, Japan Science and Technology Agency, Kawaguchi, Saitama 332-0012Yoichi KamiharaERATO-SORST, JST, c/o Frontier Research Center, Tokyo Institute of Technology, Yokohama 226-8503Masahiro HiranoERATO-SORST, JST, c/o Frontier Research Center, Tokyo Institute of Technology, Yokohama 226-8503Takaya MitsuiCREST, Japan Science and Technology Agency, Kawaguchi, Saitama 332-0012Hideo HosonoERATO-SORST, JST, c/o Frontier Research Center, Tokyo Institute of Technology, Yokohama 226-8503Makoto SetoCREST, Japan Science and Technology Agency, Kawaguchi, Saitama 332-0012
2008en
ABI

Abstract

The 57Fe M\"ossbauer spectroscopy was applied to an iron-based layered superconductor LaO0.89F0.11FeAs with a transition temperature of 26 K and its parent material LaOFeAs. Throughout the temperature range from 4.2 to 298 K, a singlet spectrum with no magnetic splitting was observed as a main component of each M\"ossbauer spectrum of the F-doped superconductor. No additional internal magnetic field was observed for the spectrum measured at 4.2 K under a magnetic field of 7 T. On the other hand, the parent LaOFeAs shows a magnetic transition at around 140 K, and this temperature is slightly lower than that of a structural phase transition from tetragonal to orthorhombic phase, which accompanies the resistivity anomaly at around 150 K. The magnetic moment is estimated to be ~0.35 $\mu$B/Fe at 4.2 K in the orthorhombic phase, and the spin disorder remains in the magnetic ordered state even at 4.2 K. The fact that no magnetic transition in LaO0.89F0.11FeAs was observed even at 4.2 K under 7 T implies a strong spin fluctuation above Tc or small magnetic moment in this system. Therefore, the present results show that the F-doping effectively suppresses the magnetic and structural transitions in the parent material and the suppression leads to emergence of superconductivity in this system.

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