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Optical observation of spin-density-wave fluctuations in Ba122 iron-based superconductors

机译:Ba122铁基超导体中自旋密度波波动的光学观察

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摘要

In iron-based superconductors, a spin-density-wave (SDW) magnetic order is suppressed with doping, and unconventional superconductivity appears in close proximity to the SDW instability. The optical response of the SDW order shows clear gap features: substantial suppression in the low-frequency optical conductivity, alongside a spectral weight transfer from low to high frequencies. Here, we study the detailed temperature dependence of the optical response in three different series of the Ba122 system [Ba_(1-x)K_xFe_2As_2, Ba(Fe_(1-x)Co_x)_2As_2, and BaFe_2(As_(1-x)P_x)_2]. Intriguingly, we find that the suppression of the low-frequency optical conductivity and spectral weight transfer appear at a temperature T~* much higher than the SDW transition temperature T_(sdw)- Since this behavior has the same optical feature and energy scale as the SDW order, we attribute it to SDW fluctuations. Furthermore, T~* is suppressed with doping, closely following the doping dependence of the nematic fluctuations detected by other techniques. These results suggest that the magnetic and nematic orders have an intimate relationship, in favor of the magnetic-fluctuation-driven nematicity scenario in iron-based superconductors.
机译:在铁基超导体中,通过掺杂抑制了自旋密度波(SDW)的磁阶,并且在SDW不稳定性附近出现了超常规的超导性。 SDW阶的光学响应显示出明显的间隙特征:低频光导率的显着抑制,以及从低频到高频的频谱权重转移。在这里,我们研究了Ba122系统的三个不同系列[Ba_(1-x)K_xFe_2As_2,Ba(Fe_(1-x)Co_x)_2As_2和BaFe_2(As_(1-x))中光学响应的​​详细温度依赖性。 P_x)_2]。有趣的是,我们发现在比SDW转变温度T_(sdw)高得多的温度T〜*处出现了对低频光导率和频谱权重转移的抑制作用,因为这种行为具有与SDW顺序,我们将其归因于SDW波动。此外,T_ *被掺杂抑制,紧随其他技术检测到的向列波动的掺杂依赖性。这些结果表明,磁和向列级有密切的关系,有利于铁基超导体中的磁波动驱动的向列情况。

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  • 来源
    《Physical Review. B, Condensed Matter》 |2016年第8期|085147.1-085147.6|共6页
  • 作者单位

    Center for High Pressure Science and Technology Advanced Research, Beijing 100094, China,Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China,LPEM, ESPCI Paris, PSL Research University, CNRS, 10 rue Vauquelin, F-75231 Paris Cedex 5, France;

    Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China,LPEM, ESPCI Paris, PSL Research University, CNRS, 10 rue Vauquelin, F-75231 Paris Cedex 5, France,Universite Pierre et Marie Curie, Sorbonne Universites, F-75005 Paris Cedex 5, France;

    Center for High Pressure Science and Technology Advanced Research, Beijing 100094, China;

    National Laboratory of Solid State Microstructures and Department of Physics, Nanjing University, Nanjing 210093, China;

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

    IRAMIS, SPEC, CEA, 91191 Gif sur Yvette, France;

    IRAMIS, SPEC, CEA, 91191 Gif sur Yvette, France;

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

    National Laboratory of Solid State Microstructures and Department of Physics, Nanjing University, Nanjing 210093, China;

    Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China;

    LPEM, ESPCI Paris, PSL Research University, CNRS, 10 rue Vauquelin, F-75231 Paris Cedex 5, France,Universite Pierre et Marie Curie, Sorbonne Universites, F-75005 Paris Cedex 5, France;

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