We theoretically investigate the transport signature of single and multiple Floquet Majorana end modes (FMEMs), appearing in an experimentally feasible setup with Rashba nanowire (NW) placed in closed proximity to a conventional $s$-wave superconductor, in the presence of an external Zeeman field. Periodic drive causes the anomalous $\pi$-modes to emerge in addition to the regular 0-modes in the driven system where the former does not exhibit any static analog. For single 0- and/or $\pi$-FMEM, differential conductance exhibits a quantized value of $2e^2/h$ while we consider the sum over all the photon sectors, supporting Floquet sum rule. We examine the stability of this summed conductance against random onsite disorder. We further investigate the summed conductance in several cases hosting multiple (more than one) 0- or $\pi$-modes at the end of the NW. In these cases, we obtain quantized values of $n_M\times 2e^2/h$ in summed differential conductance with $n_M$ being the number of modes (0 or $\pi$) localized at one end of the NW. We repeat our analysis for another experimentally realizable model system known as helical Shiba chain. Moreover, we corroborate our results by computing the differential conductance for FMEMs using nonequilibrium Green's function method. Our work opens up the possibility of studying the transport signatures of FMEMs in these realistic models.

Close

PrevNext

View figure in article

• Majorana fermions
• Topological superconductors
• Floquet systems
• Nanowires
• Landauer formula
• Nonequilibrium Green's function