Charge and spin transport through normal lead coupled to $s$-wave superconductor and a Majorana zero mode

Abstract

Zero-bias charge conductance peak (ZBCCP) is a significant symbol of Majorana zero modes (MZMs). The proximity effect of s-wave superconductor is usually demanded in the fabrication of MZMs. So in transport experiments, the system is inevitably coupled to the s-wave superconductor. Here we study how the ZBCCP is affected by coupling of the s-wave superconductor. The results show that the ZBCCP could be changed into a zero-bias valley due to the coupling of s-wave superconductor, although the conductance at the zero bias still keeps a quantized value $2e^2/h$. So it does not mean no MZM exists when no ZBCCP is experimentally observed. In addition, the spin transport is investigated. Four reflection processes (the normal reflection, spin-flip reflection, normal Andreev reflection, and equal-spin Andreev reflection) usually occur. The reflection coefficients are strongly dependent on the spin direction of the incident electron, and they may be symmetrical or Fano resonance shapes. But the spin conductance always shows a zero-bias peak with the height $e/2\pi$ regardless of the direction of the spin bias and the coupling strength of the s-wave superconductor. So measuring spin transport properties could be a more reliable method to judge the existence of MZMs.

8 pages, 5 figures

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• Spin Transport in Normal Metal-Ising Superconductor Junction
• Topological phase transition driven by magnetic field in one-dimensional topological superconductor rings
• Wavefront dislocations in graphene systems revealed by transport measurement
• Phase transitions in quantum dot-Majorana zero mode coupling systems
• Majorana modes in helical altermagnet without net magnetism and spin-orbit coupling
• Spin transport in a normal meta-altermagnetic superconducting nanowire junction
• AC/DC spin current in ferromagnet/superconductor/normal metal trilayer systems