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Published on: January 21, 2016
Upstream modes and antidots poison graphene quantum Hall effect
N Moreau1, B Brun1, S Somanchi2
1IMCN/NAPS, Université catholique de Louvain (UCLouvain), Louvain-la-Neuve, Belgium.
Topological protection in graphene's quantum Hall effect is weakened by edge antidots, which cause backscattering and breakdown. This study reveals insights into graphene edge channel vulnerability for future material development.
Area of Science:
- Condensed Matter Physics
- Materials Science
- Quantum Mechanics
Background:
- The quantum Hall effect exemplifies topological protection, utilizing 1D edge channels that prevent backscattering.
- Graphene is a promising material for studying topological properties, but its edge channels show less robustness than in semiconductors.
- Conventional Hall bar geometries limit the understanding of graphene's quantum Hall regime.
Purpose of the Study:
- To investigate the local-scale behavior of graphene's quantum Hall regime.
- To identify factors affecting the robustness of topological protection in graphene edge channels.
- To understand the influence of edge imperfections on topological breakdown.
Main Methods:
- Utilizing a scanning gate microscope to probe the graphene quantum Hall regime at a local scale.
- Conducting experiments on graphene Hall bar geometries with edge antidots.
- Employing computational simulations to complement experimental findings.
Main Results:
- Antidots along graphene edges were found to mediate backscattering towards upstream edge channels.
- This backscattering triggers a breakdown of topological protection in the quantum Hall regime.
- The local-scale exploration revealed specific vulnerabilities in graphene's edge channels.
Conclusions:
- Experimental and simulation results highlight the detrimental effect of antidots on graphene's topological protection.
- Understanding these vulnerabilities is crucial for future advancements in manipulating topologically protected edge channels.
- This research provides insights applicable to various two-dimensional crystalline materials.
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