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Observation of conductance plateau of Majorana zero modes in Fe(Te,Se)

ORAL

Abstract


Recently, iron-based superconductor turns to be a promising platform for studying Majorana quasiparticles. The sharp and isolated zero-bias conductance peaks (ZBCPs) were observed clearly by high-resolution scanning tunneling microscopy. The wavefucntion behavior of the ZBCPs and the global behavior of vortex bound states series were well studied. It implies that the observed ZBCPs are most probably Majorana zero modes (MZMs), and its topological nature renders the global π-phase shift of vortex bounds states.

There is another long-sought-after fingerprint for MZMs, i.e. 2e2/h-quantized Majorana conductance induced by resonant Andreev reflection. That resonance nature is ensured by the particle-hole equivalence of MZMs and introduces a plateau feature of zero-bias conductance at zero temperature. Due to the large energy level spacing in the vortex core, the iron-based superconductor turns to be a good platform to check that expectation. Here, I will report our recent tunnel-couple tunable STM measurement on a topological vortex of Fe(Te,Se). We find that the conductance of ZBCP has plateau behavior with its value close to or even reach 2e2/h, while other finite energy vortex bound states do not have such exotic behavior.

Ref. Zhu*, Kong*, Cao*, Chen* et al. arXiv: 1904.06124.

Presenters

  • Lingyuan Kong

    Institute of Physics, Chinese Academy of Sciences

Authors

  • Lingyuan Kong

    Institute of Physics, Chinese Academy of Sciences

  • Shiyu Zhu

    Institute of Physics, Chinese Academy of Sciences

  • Lu Cao

    Institute of Physics, Chinese Academy of Sciences

  • Hui Chen

    Institute of Physics, Chinese Academy of Sciences

  • Michal Papaj

    Massachusetts Institute of Technology, Massachusetts Institute of Technology MIT

  • Shixuan Du

    Institute of Physics, Chinese Academy of Sciences

  • Yuqing Xing

    Institute of Physics, Chinese Academy of Sciences

  • Wenyao Liu

    Chinese Academy of Sciences, Institute of Physics, Chinese Academy of Sciences

  • Dongfei Wang

    Institute of Physics, Chinese Academy of Sciences

  • Chengmin Shen

    Institute of Physics, Chinese Academy of Sciences

  • Fazhi Yang

    Institute of Physics, Chinese Academy of Sciences

  • John Schneeloch

    Brookhaven National Laboratory, Univ of Virginia, University of Virginia, Brookhaven National Lab

  • Ruidan Zhong

    Brookhaven National Laboratory, Brookhaven National Lab

  • Genda Gu

    Brookhaven National Laboratory, Condensed Matter Physics and Materials Science Division, Brookhaven National Laboratory, Brookhaven national lab, Condensed Matter Physics and Materials Science, Brookhaven National Laboratory, Brookhaven National Lab, Condensed Matter Physics and Material Science, Brookhaven National Laboratory, Upton, NY, United States, Brookhaven National Laboratories, Condensed Matter Physics and Material Science Division, Brookhaven National Laboratory

  • Liang Fu

    Massachusetts Institute of Technology, Massachusetts Institute of Technology MIT, Department of Physics, Massachusetts Institute of Technology MIT, Physics, MIT, Physics, Massachusetts Institute of Technology, MIT

  • Yuyang Zhang

    Institute of Physics, Chinese Academy of Sciences

  • Hong Ding

    Institute of Physics, Chinese Academy of Sciences, Chinese Academy of Sciences

  • Hongjun Gao

    Institute of Physics, Chinese Academy of Sciences, Institute of Physics and University of Chinese Academy of Sciences Chinese Academy of Science