Abstract

Motivated by the need to understand and simulate the ubiquitous experimentally-observed zero-bias conductance peaks in superconductor-semiconductor hybrid structures, we theoretically investigate the tunneling conductance spectra in one-dimensional nanowires in proximity to superconductors in a systematic manner taking into account several different physical mechanisms producing zero-bias conductance peaks. The mechanisms we consider are the presence of quantum dots, inhomogeneous potential, random disorder in the chemical potential, random fluctuations in the superconducting gap, and in the effective $g$ factor with the self-energy renormalization induced by the parent superconductor in both short ($L\sim1~\mu$m) and long nanowires ($L\sim3~\mu$m). We classify all foregoing theoretical results for zero-bias conductance peaks into three types: the good, the bad, and the ugly, according to the physical mechanisms producing the zero-bias peaks and their topological properties. We find that, although the topological Majorana zero modes are immune to weak disorder, strong disorder (ugly) completely suppresses topological superconductivity and generically leads to trivial zero bias peaks. Compared qualitatively with the extensive existing experimental results in the superconductor-semiconductor nanowire structures, we conclude that most current experiments are likely exploring trivial zero-bias peaks in the ugly situation dominated by strong disorder. We also study the nonlocal end-to-end correlation measurement in both the short and long wires, and point out the limitation of the nonlocal correlation in ascertaining topological properties particularly when applied to short wires. The goal of the work is to establish with a very high confidence level the real physical possibility that essentially all experimentally observed zero bias peaks in Majorana nanowires are most likely ugly.

Highlights

  • We emphasize that all zero-bias conductance peak (ZBCP) other than the good ones are topologically trivial since the ZBCPs begin to stick to zero energy in these trivial cases before the nominal topological quantum phase transition (TQPT)

  • The good ZBCPs arise from the intrinsic topological properties of the system for the Zeeman field above the topological quantum phase transition point, with the ZBCPs from the two ends of the wire showing a high level of correlations even in long wires by virtue of the nonlocal topological properties of the system

  • We show that good ZBCPs are immune to weak disorder in the chemical potential and the superconducting gap, and are robust to system parameters such as the chemical potential or Zeeman field provided one is the topological regime (i.e., Zeeman field above the TQPT value)

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Summary

Introduction

The experimental search for Majorana zero modes (MZM) [1,2,3,4,5,6,7,8,9,10,11,12,13,14,15,16,17,18,19,20,21,22,23] in the superconductor-semiconductor (SC-SM) hybrid devices has succeeded in observing many of the theoretically predicted apparent topological features, especially the quantized zero-bias conductance peak (ZBCP) in the normal-tosuperconductor (NS) tunneling spectroscopy [24,25,26,27,28,29,30,31,32,33,34,35]. The fact that no bulk signatures of a topological quantum phase transition (TQPT) (e.g., closing and reopening of a gap) have ever been reported in spite of widespread reporting of observed ZBCPs is problematic All these problems have led to alternative nontopological explanations for the experimental ZBCPs [40,41,42,43,44,45,46,47,48,49,50,51], and there have been theoretical suggestions on how to identify MZMs experimentally as well as to distinguish between topological and trivial (i.e., nontopological) ZBCPs [44,45,46,47,48].

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