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在FeSe S中,由向列相端点分隔的两种不同的超导配对态。

Two distinct superconducting pairing states divided by the nematic end point in FeSe S .

作者信息

Hanaguri Tetsuo, Iwaya Katsuya, Kohsaka Yuhki, Machida Tadashi, Watashige Tatsuya, Kasahara Shigeru, Shibauchi Takasada, Matsuda Yuji

机构信息

RIKEN Center for Emergent Matter Science, Wako, Saitama 351-0198, Japan.

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

出版信息

Sci Adv. 2018 May 25;4(5):eaar6419. doi: 10.1126/sciadv.aar6419. eCollection 2018 May.

Abstract

Unconventional superconductivity often competes or coexists with other electronic orders. In iron-based superconductors, a central issue has been the relationship between superconductivity and electronic nematicity, spontaneous breaking of the lattice rotational symmetry. Using spectroscopic-imaging scanning tunneling microscopy, we simultaneously investigated the electronic structure and the superconducting gap in FeSe S , where the nematicity diminishes above the nematic end point (NEP) at = 0.17. The nematic band structure appears as anisotropic quasiparticle-interference patterns that gradually become isotropic with increasing without anomalies at the NEP. By contrast, the superconducting gap, which is intact in the nematic phase, discontinuously shrinks above the NEP. This implies that the presence or absence of nematicity results in two distinct pairing states, whereas the pairing interaction is insensitive to the strength of nematicity.

摘要

非常规超导性常常与其他电子序相互竞争或共存。在铁基超导体中,一个核心问题一直是超导性与电子向列性(晶格旋转对称性的自发破缺)之间的关系。利用光谱成像扫描隧道显微镜,我们同时研究了FeSe S中的电子结构和超导能隙,其中向列性在 = 0.17的向列端点(NEP)以上减弱。向列能带结构表现为各向异性的准粒子干涉图案,随着 增加逐渐变得各向同性,在NEP处没有异常。相比之下,在向列相中完整的超导能隙在NEP以上会不连续地缩小。这意味着向列性的存在与否导致两种不同的配对状态,而配对相互作用对向列性的强度不敏感。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b967/5969813/83376530b6b8/aar6419-F1.jpg

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