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Nodal superconductivity coexists with low-moment static magnetism in single-crystalline tetragonal FeS: A muon spin relaxation and rotation study

机译:单晶四方FeS中节点超导与低矩静磁共存:μ子自旋弛豫和旋转研究

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摘要

We report muon spin relaxation and rotation (μSR) measurements on hydrothermally grown single crystals of superconducting tetragonal FeS. which help to clarify the controversial magnetic slate and superconducting gap symmetry of this compound. μSR time spectra were obtained from 280 K down to 0.025 K in zero field (ZF) and applied fields up to 75 mT. In ZF. the observed loss of initial asymmetry (signal amplitude) and increase of depolarization rate A_(ZF)- below 13 K indicate the onset of static magnetism, which coexists with superconductivity below T_c. TF μSR results indicate a linear temperature dependence of the superfluid density at low temperature, consistent with nodal superconductivity. The s+d-wave model gives the best fit to the observed temperature and field dependencies, and yields an in-plane penetration depth value λ_(ab)(T=0) = 241(3) nm.
机译:我们报告了对水热生长的超导四方FeS单晶体的μ自旋弛豫和旋转(μSR)测量。这有助于阐明有争议的磁性结构和该化合物的超导间隙对称性。在零场(ZF)和高达75 mT的施加场中,从280 K下降至0.025 K,获得了μSR时间谱。在ZF中。低于13 K时观察到的初始不对称性(信号幅度)损失和去极化率A_(ZF)-的增加表明静磁场的开始,这与T_c以下的超导性共存。 TFμSR结果表明低温下超流体密度与温度的线性相关性,与节流超导性一致。 s + d波模型最适合观察到的温度和磁场依赖性,并产生面内穿透深度值λ_(ab)(T = 0)= 241(3)nm。

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  • 来源
    《Physical review. B, Condensed Matter And Materals Physics》 |2018年第17期|174524.1-174524.9|共9页
  • 作者单位

    State Key Laboratory of Surface Physics, Department of Physics, Fudan University, Shanghai 200433, China;

    State Key Laboratory of Surface Physics, Department of Physics, Fudan University, Shanghai 200433, China;

    State Key Laboratory of Surface Physics, Department of Physics, Fudan University, Shanghai 200433, China;

    State Key Laboratory of Surface Physics, Department of Physics, Fudan University, Shanghai 200433, China;

    Department of Physics and Astronomy, University of California, Riverside, California 92521, USA;

    Department of Physics and Astronomy. California State University, Los Angeles, California 90032, USA;

    Department of Physics, California Slate University, Fresno, California 93740, USA;

    State Key Laboratory of Surface Physics, Department of Physics, Fudan University, Shanghai 200433, China,National High Magnetic Field Laboratory, Tallahassee, Florida 32310, USA;

    Advanced Meson Science Laboratory, RIKFN Nishina Center, Wako 351-0198, Japan;

    State Key Laboratory of Surface Physics, Department of Physics, Fudan University, Shanghai 200433, China,Collaborative Innovation Center of Advanced Microstructures. Nanjing 210093, China;

    State Key Laboratory of Surface Physics, Department of Physics, Fudan University, Shanghai 200433, China,Collaborative Innovation Center of Advanced Microstructures. Nanjing 210093, China;

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