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Coexistence of a pseudogap and a superconducting gap for the high-T_c superconductor La_(2-x)Sr_xCuO_4 studied by angle-resolved photoemission spectroscopy

机译:角分辨光发射光谱法研究高T_c超导体La_(2-x)Sr_xCuO_4的伪间隙和超导间隙的共存

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摘要

The relationship between the superconducting gap and the pseudogap has been the subject of controversies. In order to clarify this issue, we have studied the superconducting gap and pseudogap of the high-T_c superconductor La_(2-x)Sr_xCuO_4 (x = 0.10,14) by angle-resolved photoemission spectroscopy (ARPES). Through the analysis of the ARPES spectra above and below T_c, we have identified a superconducting coherence peak even in the antinodal region on top of the pseudogap of a larger energy scale. The superconducting peak energy nearly follows the pure d-wave form. The d-wave order parameter Δ_0 [defined by Δ(k) = Δ_0(cos k_xa - cos k_ya) ] for x = 0.10 and 0.14 are nearly the same, Δ_0 ~ 12-14 meV, leading to strong coupling 2Δ_0/k_BT_c ~ 10. The present result indicates that the pseudogap and the superconducting gap are distinct phenomena and can be described by the "two-gap" scenario.
机译:超导间隙和伪间隙之间的关系一直是争论的主题。为了澄清这个问题,我们通过角度分辨光发射光谱法(ARPES)研究了高T_c超导体La_(2-x)Sr_xCuO_4(x = 0.10,14)的超导间隙和拟间隙。通过分析T_c上方和下方的ARPES光谱,我们已经确定了一个超导相干峰,即使在较大能级的伪间隙顶部的反节点区域也是如此。超导峰值能量几乎遵循纯d波形式。 x = 0.10和0.14的d波阶数参数Δ_0[由Δ(k)=Δ_0(cos k_xa-cos k_ya)定义]几乎相同,Δ_0〜12-14 meV,导致强耦合2Δ_0/ k_BT_c〜 10.目前的结果表明,伪间隙和超导间隙是不同的现象,可以用“两间隙”情况来描述。

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  • 来源
    《Physical review》 |2016年第1期|014513.1-014513.5|共5页
  • 作者单位

    Department of Physics, University of Tokyo, Bunkyo-ku, Tokyo 113-0033, Japan,Graduate School of Human and Environmental Studies, Kyoto University, Sakyo-ku, Kyoto 606-8501, Japan;

    Department of Physics, University of Tokyo, Bunkyo-ku, Tokyo 113-0033, Japan;

    Department of Physics, University of Tokyo, Bunkyo-ku, Tokyo 113-0033, Japan;

    Department of Applied Physics and Stanford Synchrotron Radiation Laboratory, Stanford University, Stanford, California 94305, USA;

    Department of Applied Physics and Stanford Synchrotron Radiation Laboratory, Stanford University, Stanford, California 94305, USA;

    Department of Applied Physics and Stanford Synchrotron Radiation Laboratory, Stanford University, Stanford, California 94305, USA;

    Institute of Solid State Physics, University of Tokyo, Kashiwa 277-8581, Japan;

    Institute of Solid State Physics, University of Tokyo, Kashiwa 277-8581, Japan;

    Institute of Solid State Physics, University of Tokyo, Kashiwa 277-8581, Japan;

    Institute of Solid State Physics, University of Tokyo, Kashiwa 277-8581, Japan;

    Central Research Institute of Electric Power Industry, Yokosuka, Kanagawa 240-0196, Japan;

    Institute of Scientific and Industrial Research, Osaka University, Ibaraki, Osaka 567-0047, Japan;

    National Institute of Advanced Industrial Science and Technology, Tsukuba 305-8568, Japan;

    Department of Physics, University of Tokyo, Bunkyo-ku, Tokyo 113-0033, Japan;

    Department of Physics, University of Tokyo, Bunkyo-ku, Tokyo 113-0033, Japan;

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