Kuang Wenjun, Lopez-Polin Guillermo, Lee Hyungjun, Guinea Francisco, Whitehead George, Timokhin Ivan, Berdyugin Alexey I, Kumar Roshan Krishna, Yazyev Oleg V, Walet Niels, Principi Alessandro, Geim Andre K, Grigorieva Irina V
Department of Physics and Astronomy, University of Manchester, Manchester, M13 9PL, UK.
Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, CH-1015, Switzerland.
Adv Mater. 2021 Oct;33(39):e2103257. doi: 10.1002/adma.202103257. Epub 2021 Aug 8.
Superconductors with nontrivial band structure topology represent a class of materials with unconventional and potentially useful properties. Recent years have seen much success in creating artificial hybrid structures exhibiting the main characteristics of 2D topological superconductors. Yet, bulk materials known to combine inherent superconductivity with nontrivial topology remain scarce, largely because distinguishing their central characteristic-the topological surface states-has proved challenging due to a dominant contribution from the superconducting bulk. In this work, a highly anomalous behavior of surface superconductivity in topologically nontrivial 3D superconductor In Bi, where the surface states result from its nontrivial band structure, itself a consequence of the non-symmorphic crystal symmetry and strong spin-orbit coupling, is reported. In contrast to smoothly decreasing diamagnetic susceptibility above the bulk critical field, H , as seen in conventional superconductors, a near-perfect, Meissner-like screening of low-frequency magnetic fields well above H is observed. The enhanced diamagnetism disappears at a new phase transition close to the critical field of surface superconductivity, H . Using theoretical modeling, the anomalous screening is shown to be consistent with modification of surface superconductivity by the topological surface states. The possibility of detecting signatures of the surface states using macroscopic magnetization provides a new tool for the discovery and identification of topological superconductors.
具有非平凡能带结构拓扑的超导体代表了一类具有非常规且可能有用特性的材料。近年来,在创建展现二维拓扑超导体主要特征的人工混合结构方面取得了很大成功。然而,已知将固有超导性与非平凡拓扑相结合的块状材料仍然稀缺,这主要是因为区分其核心特征——拓扑表面态——已被证明具有挑战性,原因是超导块体的主导贡献。在这项工作中,报道了拓扑非平凡的三维超导体InBi中表面超导性的一种高度异常行为,其表面态源于其非平凡的能带结构,这本身是非简单晶格对称性和强自旋轨道耦合的结果。与传统超导体中在体临界场(H_c)之上顺磁磁化率平滑下降不同,在远高于(H_c)的情况下观察到了对低频磁场近乎完美的迈斯纳样屏蔽。增强的抗磁性在接近表面超导性临界场(H_{sc})的新相变处消失。通过理论建模表明,这种异常屏蔽与拓扑表面态对表面超导性的改变是一致的。利用宏观磁化检测表面态特征的可能性为拓扑超导体的发现和识别提供了一种新工具。