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Isotropic Quantum Griffiths Singularity in Nd0.8Sr0.2NiO2 Infinite-Layer Superconducting Thin Films
Physical Review Letters ( IF 8.1 ) Pub Date : 2024-07-17 , DOI: 10.1103/physrevlett.133.036003 Qiang Zhao 1 , Ting-Na Shao 1, 2 , Wen-Long Yang 1 , Xue-Yan Wang 1 , Xing-Yu Chen 1 , Mei-Hui Chen 1 , Fang-Hui Zhu 1 , Cheng-Xue Chen 1 , Rui-Fen Dou 1 , Chang-Min Xiong 1 , Haiwen Liu 1, 3, 4 , Jia-Cai Nie 1, 3
Physical Review Letters ( IF 8.1 ) Pub Date : 2024-07-17 , DOI: 10.1103/physrevlett.133.036003 Qiang Zhao 1 , Ting-Na Shao 1, 2 , Wen-Long Yang 1 , Xue-Yan Wang 1 , Xing-Yu Chen 1 , Mei-Hui Chen 1 , Fang-Hui Zhu 1 , Cheng-Xue Chen 1 , Rui-Fen Dou 1 , Chang-Min Xiong 1 , Haiwen Liu 1, 3, 4 , Jia-Cai Nie 1, 3
Affiliation
This work reports on the emergence of quantum Griffiths singularity (QGS) associated with the magnetic field induced superconductor-metal transition (SMT) in unconventional infinite layer superconducting thin films. The system manifests isotropic SMT features under both in-plane and perpendicular magnetic fields. Importantly, after scaling analysis of the isothermal magnetoresistance curves, the obtained effective dynamic critical exponents demonstrate divergent behavior when approaching the zero-temperature critical point , identifying the QGS characteristics. Moreover, the quantum fluctuation associated with the QGS can quantitatively explain the upturn of the upper critical field around zero temperature for both the in-plane and perpendicular magnetic fields in the phase boundary of SMT. These properties indicate that the QGS in the superconducting thin film is isotropic. Moreover, a higher magnetic field gives rise to a metallic state with the resistance-temperature relation exhibiting dependence among the 2–10 K range and dependence of resistance below 1.5 K, which is significant evidence of Kondo scattering. The interplay between isotropic QGS and Kondo scattering in the unconventional superconductor can illustrate the important role of rare region in QGS and help to uncover the exotic superconductivity mechanism in this system.
中文翻译:
Nd0.8Sr0.2NiO2 无限层超导薄膜中的各向同性量子格里菲斯奇点
这项工作报告了与非常规中磁场诱导超导体-金属转变 (SMT) 相关的量子格里菲斯奇点 (QGS) 的出现 无限层超导薄膜。该系统在平面内和垂直磁场下均表现出各向同性 SMT 特征。重要的是,在对等温磁阻曲线进行标度分析后,所获得的有效动态临界指数在接近零温临界点时表现出发散行为 ,识别 QGS 特征。此外,与QGS相关的量子涨落可以定量地解释SMT相界中面内和垂直磁场在零温度附近的上临界场的上升。这些特性表明 QGS 在 超导薄膜是各向同性的。此外,较高的磁场会产生金属态,其电阻-温度关系如下 展出 2–10 K 范围内的依赖性 电阻的依赖性低于 1.5 K,这是近藤散射的重要证据。非常规中各向同性 QGS 和近藤散射之间的相互作用 超导体可以说明稀有区域在QGS中的重要作用,并有助于揭示该系统中奇异的超导机制。
更新日期:2024-07-17
中文翻译:
Nd0.8Sr0.2NiO2 无限层超导薄膜中的各向同性量子格里菲斯奇点
这项工作报告了与非常规中磁场诱导超导体-金属转变 (SMT) 相关的量子格里菲斯奇点 (QGS) 的出现 无限层超导薄膜。该系统在平面内和垂直磁场下均表现出各向同性 SMT 特征。重要的是,在对等温磁阻曲线进行标度分析后,所获得的有效动态临界指数在接近零温临界点时表现出发散行为 ,识别 QGS 特征。此外,与QGS相关的量子涨落可以定量地解释SMT相界中面内和垂直磁场在零温度附近的上临界场的上升。这些特性表明 QGS 在 超导薄膜是各向同性的。此外,较高的磁场会产生金属态,其电阻-温度关系如下 展出 2–10 K 范围内的依赖性 电阻的依赖性低于 1.5 K,这是近藤散射的重要证据。非常规中各向同性 QGS 和近藤散射之间的相互作用 超导体可以说明稀有区域在QGS中的重要作用,并有助于揭示该系统中奇异的超导机制。