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Annealing effects on superconductivity in Rb_(0.81)Fe_(1.72)Se_2 single crystal

机译:退火对Rb_(0.81)Fe_(1.72)Se_2单晶超导性的影响

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摘要

The annealing effects on superconductivity in Rb_(0.81)Fe_(1.72)Se_2 are investigated. For as-grown single crystal and the one annealed with furnace cooling, magnetic susceptibility exhibits a weak diamagnetic transition at 30 K. Consistently, the resistivity curve only displays a small drop at 30 K and an insulating behavior at lower temperatures. These features together with scanning electron microscope (SEM) data indicate that the superconducting phase exists as clusters in insulating matrix. As for the crystal annealed with fast quenching, resistivity results reveal a T_c~(onset) ≈ 30 K and a T_c~(zero) ≈ 10 K but the susceptibility does not show diamagnetic transition until the temperature is cooled down to 10 K. SEM results show that the surface of quenched sample is more homogeneous than the one annealed with furnace cooling. We argue that the annealing at high temperature makes the coexistence of superconducting and insulating phases becomes homogeneous. Then, the fast quenching preserves this state in which percolative superconducting paths could be easily formed. In comparison, during the furnace cooling, the temperature drops slowly and results in the segregation of the superconducting phase from the insulating phase into isolated clusters.
机译:研究了退火对Rb_(0.81)Fe_(1.72)Se_2中超导性的影响。对于刚生长的单晶和经炉冷退火的单晶,磁化率在30 K时表现出弱的反磁转变。一致地,电阻率曲线在30 K时仅显示出小幅下降,并且在较低温度下表现出绝缘行为。这些特征以及扫描电子显微镜(SEM)数据表明,超导相以簇的形式存在于绝缘基质中。对于经过快速淬火退火的晶体,电阻率结果显示T_c〜(起始)≈30 K,T_c〜(零)≈10 K,但磁化率直到温度冷却至10 K时才显示出反磁性转变。结果表明,淬火样品的表面比经炉冷退火的样品更均匀。我们认为,高温退火会使超导相和绝缘相的共存变得均匀。然后,快速猝灭保持了这种状态,在该状态下可以容易地形成渗流超导路径。相比之下,在炉子冷却过程中,温度缓慢下降,并导致超导相从绝缘相分离为孤立的簇。

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  • 来源
    《Journal of Applied Physics》 |2013年第2期|17E128.1-17E128.3|共3页
  • 作者单位

    Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China;

    Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China;

    Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China;

    Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China;

    High Magnetic Field Laboratory, Hefei Institutes of Physical Science, Chinese Academy of Sciences, Hefei 230031, People's Republic of China;

    High Magnetic Field Laboratory, Hefei Institutes of Physical Science, Chinese Academy of Sciences, Hefei 230031, People's Republic of China;

    High Magnetic Field Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China;

    High Magnetic Field Laboratory, Hefei Institutes of Physical Science, Chinese Academy of Sciences, Hefei 230031, People's Republic of China;

    High Magnetic Field Laboratory, Hefei Institutes of Physical Science, Chinese Academy of Sciences, Hefei 230031, People's Republic of China;

    High Magnetic Field Laboratory, Hefei Institutes of Physical Science, Chinese Academy of Sciences, Hefei 230031, People's Republic of China,High Magnetic Field Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China;

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