Scaling of Majorana Zero-Bias Conductance Peaks (1706.07033v2)

Abstract: We report an experimental study of the scaling of zero-bias conductance peaks compatible with Majorana zero modes as a function of magnetic field, tunnel coupling, and temperature in one-dimensional structures fabricated from an epitaxial semiconductor-superconductor heterostructure. Results are consistent with theory, including a peak conductance that is proportional to tunnel coupling, saturates at $2e^2/h$, decreases as expected with field-dependent gap, and collapses onto a simple scaling function in the dimensionless ratio of temperature and tunnel coupling.

• The paper demonstrates that zero-bias peaks scale with tunnel coupling and saturate near 2e²/h, confirming key predictions of Majorana models.
• The paper reveals a direct correlation between magnetic field variations and superconducting gap modifications that facilitate Majorana mode emergence.
• The paper shows that the conductance peak follows a universal scaling function with temperature, underscoring resonant transport through zero-energy states.

Overview of "Scaling of Majorana Zero-Bias Conductance Peaks"

The paper "Scaling of Majorana Zero-Bias Conductance Peaks" presents an experimental investigation focused on the zero-bias conductance peaks (ZBPs) in one-dimensional semiconductor-superconductor hybrid structures. These structures leverage epitaxial heterostructures, which potentially support Majorana zero modes (MZMs), a theoretical construct with applications in topological quantum computation. The researchers aim to elucidate the dependence of these ZBPs on parameters such as magnetic field, tunnel coupling, and temperature.

Experimental Design and Methodology

The research employs devices based on InAs/Al heterostructures, where an InAs quantum well is interfaced epitaxially with aluminum, forming superconductor-insulator-normal (SIN) junctions. The experimental setup allows precise control over gate voltages that modulate the chemical potential and tunnel barrier, thus affecting tunneling conductance. Utilizing a dilution refrigerator, low-frequency lock-in techniques are applied, and data is gathered across a range of temperatures to explore how ZBPs evolve under varying conditions.

Key Findings

1. Consistency with Theoretical Models:
   • The observed ZBP conductance is shown to scale proportionately with tunnel coupling, saturating at approximately $2e^2/h$, aligning with predictions for ideal MZMs.
   • There is a pronounced temperature dependence that fits well to models considering resonant transport through zero-energy modes.
2. Magnetic Field Dependence:
   • The observed ZBPs correlate with the magnetic field, which is conducive to inducing MZMs, with the field affecting the induced superconducting gap and thereby modifying the ZBP amplitude.
3. Temperature and Tunnel Coupling Scaling:
   • The conductance peak shows robust scaling behavior mapped onto a universal function of the temperature-to-broadening ratio, emphasizing the role of tunnel coupling and temperature in defining the peak’s characteristics.

Implications and Future Directions

The implications of this paper are primarily in the field of topological quantum computation, where MZMs are envisioned as fault-tolerant qubits. The results highlight the practical considerations of temperature and tunnel coupling in optimizing ZBP signatures for device applications. Furthermore, while the experimentally observed conductance characteristics are compatible with Majorana interpretations, they do not unequivocally rule out alternative nontopological explanations. This complexity suggests that future research should continue refining the methodologies for unambiguously differentiating between Majorana-induced and trivial ZBP scenarios.

Conclusions

The paper underscores a critical advancement in the characterization and control of ZBPs, aligning experimental outcomes with theoretical expectations of MZM behavior. While the findings are promising, the complexity of distinguishing MZMs from potential trivial states necessitates further experimental scrutiny and innovation. Looking ahead, efforts should be dedicated to exploring multimode transport dynamics and potential effects of disorder, facilitating the next steps towards robust MZM implementations for quantum technologies.