Related Experiment Video
Updated: Jun 8, 2026

11:24
Optimized Fabrication Procedure for High-Quality Graphene-based Moiré Superlattice Devices
Published on: July 11, 2025
Tunable Luttinger liquid physics in biased bilayer graphene
Matthew Killi1, Tzu-Chieh Wei, Ian Affleck
1Department of Physics, University of Toronto, Toronto, Ontario, M5S1A7, Canada.
Physical Review Letters
|September 28, 2010
Summary
Electronically gated bilayer graphene exhibits tunable semiconducting properties. Applying a spatially varying bias creates one-dimensional chiral modes that behave as a strongly interacting Tomonaga-Luttinger liquid.
Area of Science:
- Condensed Matter Physics
- Materials Science
- Quantum Mechanics
Background:
- Bilayer graphene under uniform bias acts as a tunable gap semiconductor.
- Spatially varying bias is key to creating novel electronic states.
Purpose of the Study:
- Investigate the behavior of one-dimensional (1D) chiral modes in bilayer graphene under spatially varying bias.
- Characterize the electronic interactions and properties of these 1D modes.
Main Methods:
- Theoretical modeling of bilayer graphene with a spatially varying interlayer bias.
- Incorporation of Coulomb repulsion and gate voltage-dependent electronic properties.
- Analysis of low-energy wave function spread and electron interactions.
Main Results:
- Spatially varying bias induces 1D chiral modes localized at the bias domain wall.
- Forward scattering Coulomb repulsion is the dominant interaction for these 1D electrons.
- These modes exhibit characteristics of a strongly interacting Tomonaga-Luttinger liquid.
Conclusions:
- The 1D chiral modes in bilayer graphene behave as a Tomonaga-Luttinger liquid.
- The system displays three distinct mode velocities and a bias-dependent Luttinger parameter.
- Experimental signatures for these strongly interacting 1D modes are discussed.
Related Concept Videos
Biasing of Metal-Semiconductor Junctions
Biasing metal-semiconductor junctions involves applying a voltage across the junction. Specifically, the metal is connected to a voltage source, while the semiconductor is grounded. This technique is essential for controlling the direction and magnitude of current flow in electronic devices, including diodes, transistors, and photovoltaic cells.
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
Biasing of FET
Biasing a Junction Field Effect Transistor (JFET) is crucial for setting operational parameters and ensuring efficient functioning in electronic circuits. JFETs are characterized by using a single carrier type in N-channel or P-channel configurations, where the channel is surrounded by PN junctions. These junctions are central to the device's ability to control current flow.
In an N-channel JFET, the structure consists of N-type material forming the channel on a P-type substrate, with the gate...
In an N-channel JFET, the structure consists of N-type material forming the channel on a P-type substrate, with the gate...
The Electrical Double Layer
In the region where two bulk phases meet, an intricate electric charge distribution arises due to charge transfer, ion adsorption, molecular orientation, and charge distortion. This complex distribution is commonly referred to as the electrical double layer.When a solid electrode interfaces with ions in an electrolyte solution, the speed of electron transfer dictates the rates of oxidation and reduction. The electrode acquires a charge through the escape of atoms into the solution as cations or...
Debye–Huckel–Onsager Conductance Equation
The Debye-Hückel-Onsager equation is a cornerstone of physical chemistry, providing a method to determine the molar conductance (Λm) and molar conductance at infinite dilution (Λ°m) for uni-univalent electrolytes.Uni-univalent electrolytes are electrolytes that dissociate in solution to produce one cation with a +1 charge and one anion with a –1 charge per formula unit.This equation addresses two crucial phenomena: the asymmetry effect and the electrophoretic effect. According to this equation,...
Bewley Lattice Diagram
The Bewley lattice diagram, developed by L. V. Bewley, effectively organizes the reflections occurring during transmission-line transients. It visually represents how voltage waves propagate and reflect within a transmission line, making it easier to understand the complex interactions that occur.
Biasing of P-N Junction
The operation of a p-n junction diode involves various biasing conditions, including forward bias, reverse bias, and equilibrium.
In equilibrium, no external voltage is applied across the p-n junction. The depletion region is formed at the junction interface due to the diffusion of carriers, which leaves behind charged dopants, acceptors on the p-side, and donors on the n-side. These immobile charges create an electric field that prevents further diffusion of carriers. The related energy band...
In equilibrium, no external voltage is applied across the p-n junction. The depletion region is formed at the junction interface due to the diffusion of carriers, which leaves behind charged dopants, acceptors on the p-side, and donors on the n-side. These immobile charges create an electric field that prevents further diffusion of carriers. The related energy band...

