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首页> 外文期刊>Physical review >Doping evolution of the quasiparticle excitations in heavily hole-doped Ba_(1-x)K_xFe_2As_2: A possible superconducting gap with sign-reversal between hole pockets
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Doping evolution of the quasiparticle excitations in heavily hole-doped Ba_(1-x)K_xFe_2As_2: A possible superconducting gap with sign-reversal between hole pockets

机译:重空穴掺杂的Ba_(1-x)K_xFe_2As_2中准粒子激发的掺杂演化:空穴腔之间可能发生带符号反转的超导间隙

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摘要

To gain insight into the unconventional superconductivity of Fe pnictides with no electron pockets, we measure the thermal conductivity k and penetration depth X in the heavily hole-doped regime of Ba_(1-x)K_xFe_2As_2. The residual thermal conductivity (κ/ T)_T→0 k and T dependence of λ consistently indicate the fully gapped superconductivity at x = 0.76 and the (line) nodal superconductivity at higher hole concentrations. The magnitude of κ/T_T_c|T→0 κ and the slope of λ(T) at low temperatures, both of which are determined by the properties of the low-energy excitations, exhibit a highly unusual nonmonotonic x dependence. These results indicate a dramatic change of the nodal characteristics in a narrow doping range. We suggest that the observed x dependence is naturally explained by a doping crossover of the gap function between the s-wave states with and without sign reversal between Γ-centered hole pockets.
机译:为了深入了解没有电子腔的Fe肽的非常规超导性,我们在重掺杂Ba_(1-x)K_xFe_2As_2的情况下测量了热导率k和穿透深度X。剩余的热导率(κ/ T)_T→0 k和λ的T依赖性始终表明在x = 0.76时完全空缺的超导性和在较高空穴浓度下的(线)节点超导性。 κ/ T_T_c | T→0κ的大小和低温下的λ(T)的斜率都由低能激发的性质决定,它们表现出非常不寻常的非单调x依赖性。这些结果表明在窄掺杂范围内节点特性发生了巨大变化。我们建议,观察到的x依赖性自然可以通过s波状态之间的间隙函数的掺杂交叉来解释,在以Γ为中心的空穴之间有和没有符号反转。

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  • 来源
    《Physical review》 |2014年第11期|115112.1-115112.5|共5页
  • 作者单位

    Department of Physics, Kyoto University, Kyoto 606-8502, Japan;

    Department of Physics, Kyoto University, Kyoto 606-8502, Japan;

    Department of Physics, Kyoto University, Kyoto 606-8502, Japan;

    Department of Physics, Kyoto University, Kyoto 606-8502, Japan;

    Department of Physics, Kyoto University, Kyoto 606-8502, Japan;

    Department of Physics, Kyoto University, Kyoto 606-8502, Japan;

    Department of Physics, Kyoto University, Kyoto 606-8502, Japan;

    Department of Physics, Kyoto University, Kyoto 606-8502, Japan ,Institute for Solid State Physics, University of Tokyo, Chiba 277-8581 Japan;

    Department of Physics, Chiba University, Chiba 263-8522, Japan;

    Department of Physics, Chiba University, Chiba 263-8522, Japan;

    National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568, Japan;

    National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568, Japan;

    National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568, Japan;

    National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568, Japan;

    National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568, Japan;

    National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568, Japan;

    Department of Physics, Montana State University, Bozeman, Montana 59717, USA;

    Department of Physics, Kyoto University, Kyoto 606-8502, Japan ,Department of Advanced Materials Science, University of Tokyo, Chiba 277-8561, Japan;

    Department of Physics, Kyoto University, Kyoto 606-8502, Japan;

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  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

    pairing symmetries (other than s-wave); superconductivity phase diagrams;

    机译:配对对称性(s波除外);超导相图;

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