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首页> 外文期刊>Physical review letters >Mapping the Electronic Structure of Each Ingredient Oxide Layer of High-T-c Cuprate Superconductor Bi2Sr2CaCu2O8+delta
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Mapping the Electronic Structure of Each Ingredient Oxide Layer of High-T-c Cuprate Superconductor Bi2Sr2CaCu2O8+delta

机译:高T-c铜酸盐超导体Bi2Sr2CaCu2O8 +δ的每个成分氧化物层的电子结构图

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摘要

Understanding the mechanism of high transition temperature (T-c) superconductivity in cuprates has been hindered by the apparent complexity of their multilayered crystal structure. Using a cryogenic scanning tunneling microscopy (STM), we report on layer-by-layer probing of the electronic structures of all ingredient planes (BiO, SrO, CuO2) of Bi2Sr2CaCu2O8+delta superconductor prepared by argon-ion bombardment and annealing technique. We show that the well-known pseudogap (PG) feature observed by STM is inherently a property of the BiO planes and thus irrelevant directly to Cooper pairing. The SrO planes exhibit an unexpected van Hove singularity near the Fermi level, while the CuO2 planes are exclusively characterized by a smaller gap inside the PG. The small gap becomes invisible near T-c, which we identify as the superconducting gap. The above results constitute severe constraints on any microscopic model for high T-c superconductivity in cuprates.
机译:了解铜酸盐中的高转变温度(T-c)超导性的机理已被其多层晶体结构的表面复杂性所阻碍。使用低温扫描隧道显微镜(STM),我们报告了通过氩离子轰击和退火技术制备的Bi2Sr2CaCu2O8 +δ超导体的所有成分平面(BiO,SrO,CuO2)的电子结构的逐层探测。我们表明,由STM观察到的众所周知的伪间隙(PG)特征固有地是BiO平面的属性,因此与Cooper配对直接无关。 SrO平面在费米能级附近表现出出乎意料的范霍夫奇异性,而CuO2平面则仅以PG内部较小的间隙为特征。小间隙在T-c附近变得不可见,我们将其识别为超导间隙。以上结果构成了任何微观模型对铜酸盐中高T-c超导性的严格约束。

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  • 来源
    《Physical review letters》 |2015年第23期|237002.1-237002.5|共5页
  • 作者单位

    Tsinghua Univ, Dept Phys, State Key Lab Low Dimens Quantum Phys, Beijing 100084, Peoples R China;

    Tsinghua Univ, Dept Phys, State Key Lab Low Dimens Quantum Phys, Beijing 100084, Peoples R China;

    Tsinghua Univ, Dept Phys, State Key Lab Low Dimens Quantum Phys, Beijing 100084, Peoples R China;

    Tsinghua Univ, Dept Phys, State Key Lab Low Dimens Quantum Phys, Beijing 100084, Peoples R China;

    Tsinghua Univ, Dept Phys, State Key Lab Low Dimens Quantum Phys, Beijing 100084, Peoples R China;

    Tsinghua Univ, Dept Phys, State Key Lab Low Dimens Quantum Phys, Beijing 100084, Peoples R China|Collaborat Innovat Ctr Quantum Matter, Beijing 100084, Peoples R China;

    Tsinghua Univ, Dept Phys, State Key Lab Low Dimens Quantum Phys, Beijing 100084, Peoples R China|Collaborat Innovat Ctr Quantum Matter, Beijing 100084, Peoples R China;

    Tsinghua Univ, Dept Phys, State Key Lab Low Dimens Quantum Phys, Beijing 100084, Peoples R China|Collaborat Innovat Ctr Quantum Matter, Beijing 100084, Peoples R China;

    Brookhaven Natl Lab, Condensed Matter Phys & Mat Sci Dept, Upton, NY 11973 USA;

    Brookhaven Natl Lab, Condensed Matter Phys & Mat Sci Dept, Upton, NY 11973 USA;

    Brookhaven Natl Lab, Condensed Matter Phys & Mat Sci Dept, Upton, NY 11973 USA;

    Tsinghua Univ, Dept Phys, State Key Lab Low Dimens Quantum Phys, Beijing 100084, Peoples R China|Collaborat Innovat Ctr Quantum Matter, Beijing 100084, Peoples R China;

    Tsinghua Univ, Dept Phys, State Key Lab Low Dimens Quantum Phys, Beijing 100084, Peoples R China|Collaborat Innovat Ctr Quantum Matter, Beijing 100084, Peoples R China;

    Tsinghua Univ, Dept Phys, State Key Lab Low Dimens Quantum Phys, Beijing 100084, Peoples R China|Collaborat Innovat Ctr Quantum Matter, Beijing 100084, Peoples R China;

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