当前位置: X-MOL 学术Adv. Mater. › 论文详情
Our official English website, www.x-mol.net, welcomes your feedback! (Note: you will need to create a separate account there.)
Evidence for Anisotropic Superconductivity Beyond Pauli Limit in Infinite-Layer Lanthanum Nickelates
Advanced Materials ( IF 27.4 ) Pub Date : 2023-05-26 , DOI: 10.1002/adma.202303400
Wenjie Sun 1 , Yueying Li 1 , Ruxin Liu 2 , Jiangfeng Yang 1 , Jiayi Li 1 , Wei Wei 3 , Gangjian Jin 4 , Shengjun Yan 1 , Haoying Sun 1 , Wei Guo 1 , Zhengbin Gu 1 , Zengwei Zhu 5 , Yue Sun 3 , Zhixiang Shi 3 , Yu Deng 1 , Xuefeng Wang 2 , Yuefeng Nie 1
Affiliation  

After being expected to be a promising analog to cuprates for decades, superconductivity has recently been discovered in infinite-layer nickelates, providing new opportunities to explore mechanisms of high-temperature superconductivity. However, in sharp contrast to the single-band and anisotropic superconductivity in cuprates, nickelates exhibit a multi-band electronic structure and an unexpected isotropic superconductivity as reported recently, which challenges the cuprate-like picture in nickelates. Here, it is shown that strong anisotropic magnetotransport behaviors exist in La-based nickelate films with enhanced crystallinity and superconductivity ( T c onset $T_{\rm{c}}^{{\rm{onset}}}$ = 18.8 K, T c zero $T_{\rm{c}}^{{\rm{zero}}}$ = 16.5 K). The upper critical fields are anisotropic and violate the estimated Bardeen–Cooper–Schrieffer (BCS) Pauli limit ( H Pauli , μ = 1 μ B = 1.86 × T c , H = 0 ${H}_{\mathrm{Pauli},\mu =1{\mu}_{B}}=1.86\ensuremath{\times{}}{T}_{\mathrm{c},H=0}$ ) for in-plane magnetic fields. Moreover, the anisotropic superconductivity is further manifested by the cusp-like peak of the angle-dependent Tc and the vortex motion anisotropy under external magnetic fields.

中文翻译:

无限层镍酸镧中各向异性超导超出泡利极限的证据

几十年来人们一直期望成为铜酸盐的有前途的类似物,最近在无限层镍酸盐中发现了超导性,为探索高温超导机制提供了新的机会。然而,与铜酸盐中的单能带和各向异性超导性形成鲜明对比的是,镍酸盐表现出多能带电子结构和意想不到的各向同性超导性,这对镍酸盐中类似铜酸盐的图像提出了挑战。研究表明,具有增强结晶度和超导性的 La 基镍酸盐薄膜中存在强各向异性磁输运行为( 时间 C 发作 $T_{\rm{c}}^{{\rm{开始}}}$ = 18.8 K, 时间 C $T_{\rm{c}}^{{\rm{零}}}$ = 16.5 K)。上临界场是各向异性的,违反了估计的 Bardeen-Cooper-Schrieffer (BCS) Pauli 极限( H 泡利 , μ = 1 μ = 1.86 × 时间 C , H = 0 ${H}_{\mathrm{泡利},\mu =1{\mu}_{B}}=1.86\ensuremath{\times{}}{T}_{\mathrm{c},H=0} $ )对于平面内磁场。此外,各向异性超导性进一步通过与角度相关的T c的尖峰和外部磁场下的涡旋运动各向异性来体现。
更新日期:2023-05-26
down
wechat
bug