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Superconductivity above 100 K in single-layer FeSe films on doped SrTiO_3

机译:掺杂SrTiO_3上单层FeSe薄膜中100 K以上的超导

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Recent experiments on FeSe films grown on SrTiO_3 (STO) suggest that interface effects can be used as a means to reach superconducting critical temperatures (T_c) of up to 80 K (ref. 1). This is nearly ten times the T_c of bulk FeSe and higher than the record value of 56 K for known bulk Fe-based superconductors. Together with recent studies of superconductivity at oxide heterostructure interfaces, these results rekindle the long-standing idea that electron pairing at interfaces between two different materials can be tailored to achieve high-temperature superconductivity. Subsequent angle-resolved photoemission spectroscopy measurements of the FeSe/STO system revealed an electronic structure distinct from bulk FeSe (refs 13,14), with an energy gap vanishing at around 65 K. However, ex situ electrical transport measurements have so far detected zero resistance-the key experimental signature of superconductivity-only below 30 K. Here, we report the observation of superconductivity with T_c above 100 K in the FeSe/STO system by means of in situ four-point probe electrical transport measurements. This finding confirms FeSe/STO as an ideal material for studying high-T_c superconductivity.
机译:最近在SrTiO_3(STO)上生长的FeSe薄膜上的实验表明,界面效应可用作达到高达80 K的超导临界温度(T_c)的手段(参考资料1)。这几乎是块状FeSe的T_c的十倍,并且高于已知的块状Fe基超导体的56 K的记录值。与最近对氧化物异质结构界面处的超导性的研究一起,这些结果重新激发了长期存在的观念,即可以对两种不同材料之间的界面处的电子配对进行定制以实现高温超导性。随后的FeSe / STO系统的角分辨光发射光谱测量显示出不同于块状FeSe的电子结构(参考文献13,14),能隙在65 K左右消失。然而,非原位电迁移测量迄今检测到零电阻-超导性的关键实验信号-仅在30 K以下。在这里,我们通过原位四点探针电迁移测量报告了在FeSe / STO系统中T_c高于100 K的超导性。这一发现证实了FeSe / STO是研究高T_c超导性的理想材料。

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  • 来源
    《Nature Materials》 |2015年第3期|285-289|共5页
  • 作者单位

    Key Laboratory of Artificial Structures and Quantum Control (Ministry of Education), Department of Physics and Astronomy, Shanghai Jiao Tong University, 800 Dongchuan Road, Shanghai 200240, China;

    Key Laboratory of Artificial Structures and Quantum Control (Ministry of Education), Department of Physics and Astronomy, Shanghai Jiao Tong University, 800 Dongchuan Road, Shanghai 200240, China;

    Key Laboratory of Artificial Structures and Quantum Control (Ministry of Education), Department of Physics and Astronomy, Shanghai Jiao Tong University, 800 Dongchuan Road, Shanghai 200240, China,Collaborative Innovation Center of Advanced Microstructures, Nanjing 210093, China;

    Key Laboratory of Artificial Structures and Quantum Control (Ministry of Education), Department of Physics and Astronomy, Shanghai Jiao Tong University, 800 Dongchuan Road, Shanghai 200240, China,Collaborative Innovation Center of Advanced Microstructures, Nanjing 210093, China;

    Key Laboratory of Artificial Structures and Quantum Control (Ministry of Education), Department of Physics and Astronomy, Shanghai Jiao Tong University, 800 Dongchuan Road, Shanghai 200240, China,Collaborative Innovation Center of Advanced Microstructures, Nanjing 210093, China;

    Department of Physics, Tsinghua University, Beijing 100084, China;

    Key Laboratory of Artificial Structures and Quantum Control (Ministry of Education), Department of Physics and Astronomy, Shanghai Jiao Tong University, 800 Dongchuan Road, Shanghai 200240, China,Collaborative Innovation Center of Advanced Microstructures, Nanjing 210093, China,Department of Physics and Materials Research Institute, Pennsylvania State University, University Park, Pennsylvania 16802, USA;

    Key Laboratory of Artificial Structures and Quantum Control (Ministry of Education), Department of Physics and Astronomy, Shanghai Jiao Tong University, 800 Dongchuan Road, Shanghai 200240, China,Collaborative Innovation Center of Advanced Microstructures, Nanjing 210093, China;

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