Spin Ordering in LaFeAsO and Its Suppression in Superconductor LaFeAsO0.89F0.11 Probed by Mossbauer Spectroscopy

被引:88
作者
Kitao, Shinji [1 ,2 ]
Kobayashi, Yasuhiro [1 ,2 ]
Higashitaniguchi, Satoshi [1 ,2 ]
Saito, Makina [1 ,2 ]
Kamihara, Yoichi [3 ]
Hirano, Masahiro [3 ]
Mitsui, Takaya [2 ,4 ]
Hosono, Hideo [3 ,5 ]
Seto, Makoto [1 ,2 ,4 ]
机构
[1] Kyoto Univ, Inst Res Reactor, Osaka 5900494, Japan
[2] Japan Sci & Technol Agcy, CREST, Kawaguchi, Saitama 3320012, Japan
[3] Tokyo Inst Technol, Frontier Res Ctr, JST, ERATO SORST, Yokohama, Kanagawa 2268503, Japan
[4] Japan Atom Energy Agcy, Sayo, Hyogo 6795148, Japan
[5] Tokyo Inst Technol, Mat & Struct Lab, Yokohama, Kanagawa 2268503, Japan
关键词
Fe-57 Mossbauer spectroscopy; LaFeAsO; LaFeAsO1-xFx; F doping; superconductivity; magnetic moment;
D O I
10.1143/JPSJ.77.103706
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
Fe-57 Mossbauer spectroscopy was applied to an iron-based layered superconductor LaFeAsO0.89F0.11 with a transition temperature of 26 K and to its parent material LaFeAsO. Throughout the temperature range from 4.2 to 298 K, a singlet pattern with no magnetic splitting was observed in the Mossbauer spectrum of the F-doped superconductor. Furthermore, 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, magnetically split spectra were observed in the parent LaFeAsO below 140 K, and this temperature is slightly lower than that of a structural phase transition from tetragonal to orthorhombic phase, which accompanies the electrical resistivity anomaly at around 150 K The magnetic moment is estimated to be similar to 0.35 mu(B)/Fe from the internal magnetic field of 5.3 T at 4.2 K in the orthorhombic phase, and the spin disorder appears to remain in the magnetically ordered state even at 4.2 K. The lack of a magnetic transition in LaFeAsO0.89F0.11 down to 4.2 K Suggests that this system exhibits a paramagnetic state or that the magnetic moment is small. The present results show that F doping effectively suppresses the magnetic and structural transitions in the parent material, leading to the emergence of superconductivity in the F-doped system.
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页数:3
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