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在非中心对称的 LaIr 中存在 s 波超导性的证据。

Evidence of s-wave superconductivity in the noncentrosymmetric LaIr.

机构信息

College of Science, Nanjing University of Posts and Telecommunications, Nanjing, 210023, China.

Advanced Functional Materials Lab and Department of Physics, Changshu Institute of Technology, Changshu, 215500, China.

出版信息

Sci Rep. 2018 Jan 12;8(1):651. doi: 10.1038/s41598-017-19042-x.

Abstract

Superconductivity in noncentrosymmetric compounds has attracted sustained interest in the last decades. Here we present a detailed study on the transport, thermodynamic properties and the band structure of the noncentrosymmetric superconductor La Ir (T  ~ 2.3 K) that was recently proposed to break the time-reversal symmetry. It is found that LaIr displays a moderately large electronic heat capacity (Sommerfeld coefficient γ  ~ 53.1 mJ/mol K) and a significantly enhanced Kadowaki-Woods ratio (KWR 32 μΩ cm mol K J) that is greater than the typical value (10 μΩ cm mol K J) for strongly correlated electron systems. The upper critical field H was seen to be nicely described by the single-band Werthamer-Helfand-Hohenberg model down to very low temperatures. The hydrostatic pressure effects on the superconductivity were also investigated. The heat capacity below T reveals a dominant s-wave gap with the magnitude close to the BCS value. The first-principles calculations yield the electron-phonon coupling constant λ = 0.81 and the logarithmically averaged frequency ω  = 78.5 K, resulting in a theoretical T  = 2.5 K, close to the experimental value. Our calculations suggest that the enhanced electronic heat capacity is more likely due to electron-phonon coupling, rather than the electron-electron correlation effects. Collectively, these results place severe constraints on any theory of exotic superconductivity in this system.

摘要

在过去的几十年中,非中心对称化合物中的超导性一直引起人们的持续兴趣。在这里,我们对最近提出的打破时间反转对称性的非中心对称超导体 LaIr(T ~ 2.3K)的输运、热力学性质和能带结构进行了详细研究。结果表明,LaIr 表现出中等大小的电子热容(Sommerfeld 系数 γ ~ 53.1 mJ/mol K)和显著增强的 Kadowaki-Woods 比(KWR 32 μΩ cm mol K J),大于强关联电子系统的典型值(10 μΩ cm mol K J)。上临界场 H 很好地符合单带 Werthamer-Helfand-Hohenberg 模型,直至非常低的温度。还研究了静水压力对超导性的影响。在 T 以下,热容显示出主导的 s 波能隙,其大小接近 BCS 值。第一性原理计算得出电子-声子耦合常数 λ = 0.81 和对数平均频率 ω = 78.5 K,导致理论 T = 2.5 K,接近实验值。我们的计算表明,增强的电子热容更可能归因于电子-声子耦合,而不是电子-电子相关效应。总的来说,这些结果对该系统中任何奇异超导理论都提出了严格的限制。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b090/5766628/5cb02118433f/41598_2017_19042_Fig1_HTML.jpg

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