Related Experiment Video
Updated: Sep 4, 2025

Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform
Published on: August 2, 2019
Interplay between topological valley and quantum Hall edge transport.
Fabian R Geisenhof1, Felix Winterer1, Anna M Seiler1,2
1Physics of Nanosystems, Department of Physics, Ludwig-Maximilians-Universität München, Munich, Germany.
Topological domain wall states and quantum Hall edge transport in bilayer graphene were studied. Their interplay shows suppressed transport at high magnetic fields, suggesting domain walls may not be topological.
Area of Science:
- Condensed Matter Physics
- Materials Science
Background:
- Topologically protected states are typically created using magnetic fields in 2D electron gases, forming quantum Hall edge channels.
- Bilayer graphene exhibits topologically protected states at stacking domain walls, even without magnetic fields.
- The interplay between these two types of topological states is not well understood.
Purpose of the Study:
- Investigate the interplay between topological domain wall states and quantum Hall edge transport.
- Focus on the eight-fold degenerate zeroth Landau level in high-quality suspended bilayer graphene.
Main Methods:
- Utilized high-quality suspended bilayer graphene.
- Applied varying magnetic fields to observe transport phenomena.
- Measured two-terminal conductance across distinct quantum Hall states.
Main Results:
- Two-terminal conductance remained constant at low magnetic fields due to channel trading between domain walls and device edges.
- Observed transport suppression at domain walls at high magnetic fields.
- Evidence suggests the emergence of spectral minigaps at domain walls.
Conclusions:
- Stacking domain walls in bilayer graphene may not represent true topological domain walls in the order parameter.
- The observed transport suppression indicates a deviation from expected topological behavior at higher magnetic fields.
Related Concept Videos
The Hall Effect
Electric Field at the Surface of a Conductor
In the 19th century, Michael Faraday conducted the famous ice pail experiment to prove that the charges always reside on the surface of a conductor. The experimental set-up consists of a conducting uncharged container mounted on an insulating stand. The outer surface of the container is...
Electric Field of Parallel Conducting Plates
Consider a cross-section of a thin, infinite conducting plate having a positive charge. For such a large thin plate, as the thickness of the plate tends to zero, the positive charges lie on the plate's two large faces. Without an external electric...
Electric Field Inside a Conductor
Suppose a piece of metal is placed near a positive charge. The free electrons in the metal are attracted to the external positive charge and migrate freely toward that region. This region then...
P-N junction
Biasing of Metal-Semiconductor Junctions
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...

