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Majorana fermions in ferromagnetic chains on the surface of bulk spin-orbit coupled s-wave superconductors

机译:自旋轨道耦合 s 波超导体表面铁磁链中的马约拉那费米子

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Majorana fermion (MF) excitations in solid state system have non-Abelian statistics which is essential for topological quantum computation. Previous proposals to realize MF, however, generally requires fine-tuning of parameters. Here we explore a platform which avoids the fine-tuning problem, namely a ferromagnetic chain deposited on the surface of a spin-orbit coupled s -wave superconductor. We show that it generically supports zero-energy topological MF excitations near the two ends of the chain with minimal fine-tuning. Depending on the strength of the ferromagnetic moment in the chain, the number of MFs at each end, n , can be either one or two, and should be revealed by a robust zero-bias peak (ZBP) of height 2 ne 2/ h in scanning tunneling microscopy (STM) measurements which would show strong (weak) signals at the ends (middle) of the chain. The role of an approximate chiral symmetry which gives an integer topological invariant to the system is discussed.
机译:固态系统中的马约拉那费米子(MF)激发具有非阿贝尔统计量,这对于拓扑量子计算至关重要。但是,以前实现MF的建议通常需要对参数进行微调。在这里,我们探索了一个避免微调问题的平台,即沉积在自旋轨道耦合s型超导体表面的铁磁链。我们表明,它通常以最小的微调来支持链两端附近的零能量拓扑MF激发。取决于链中铁磁矩的强度,两端的MF数n可以为1或2,并且应通过高度为2 ne的稳健的零偏峰(ZBP)来揭示在扫描隧道显微镜(STM)测量中为2 / h,这将在链的末端(中间)显示强(弱)信号。讨论了使系统具有整数拓扑不变性的近似手性对称性的作用。

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