Related Experiment Video
Updated: Mar 10, 2026

10:36
Advanced Experimental Methods for Low-temperature Magnetotransport Measurement of Novel Materials
Published on: January 21, 2016
11.4K
Quantum Hall effect in epitaxial graphene with permanent magnets
F D Parmentier1, T Cazimajou1, Y Sekine2
1SPEC, CEA, CNRS, Université Paris-Saclay, CEA Saclay 91191 Gif-sur-Yvette cedex, France.
Scientific Reports
|December 7, 2016
Summary
Researchers observed the quantum Hall effect (QHE) in epitaxial graphene using only permanent magnets, a first. This cost-effective method makes QHE research in graphene more accessible for future applications.
Area of Science:
- Condensed Matter Physics
- Materials Science
Background:
- The quantum Hall effect (QHE) is a key phenomenon in condensed matter physics, typically observed in 2D electron systems under strong magnetic fields and low temperatures.
- Conventional QHE experiments often rely on expensive and complex superconducting magnets, limiting accessibility for research and education.
Purpose of the Study:
- To demonstrate the observation of the quantum Hall effect in epitaxial graphene using only permanent magnets.
- To explore the feasibility of a cost-effective experimental setup for studying QHE in graphene.
Main Methods:
- Epitaxial graphene grown on silicon carbide (SiC) was used as the 2D electron system.
- Commercial Neodymium-Iron-Boron (NdFeB) permanent magnets were employed to generate a sufficiently large and homogeneous magnetic field at low temperatures.
- A top gate was utilized to tune the electronic properties and control edge channel chirality.
Main Results:
- The quantum Hall effect was successfully observed in epitaxial graphene at Landau level filling factors of ±2, comparable to results obtained with superconducting magnets.
- The chirality of the QHE edge channels was demonstrated to be tunable via the top gate.
- The experiment confirmed the formation of well-developed quantum Hall states.
Conclusions:
- The use of permanent magnets provides a significantly more affordable and accessible method for observing the QHE in graphene.
- This breakthrough lowers the barrier for QHE research in graphene, paving the way for broader scientific investigation and potential technological applications.
- The findings highlight the potential of graphene-based systems for fundamental physics studies and device development.
Related Concept Videos
The Hall Effect
4.8K
Edwin H. Hall, in the year 1879, devised an experiment that could be used to identify the polarity of the predominant charge carriers in a conducting material. From a historical perspective, this experiment was the first to demonstrate that the charge carriers in most metals are negative.
4.8K
Magnetic Fields
7.7K
A moving charge or a current creates a magnetic field in the surrounding space, in addition to its electric field. The magnetic field exerts a force on any other moving charge or current that is present in the field. Like an electric field, the magnetic field is also a vector field. At any position, the direction of the magnetic field is defined as the direction in which the north pole of a compass needle points.
A magnetic field is defined by the force that a charged particle experiences...
A magnetic field is defined by the force that a charged particle experiences...
7.7K
π Electron Effects on Chemical Shift: Overview
1.8K
An applied magnetic field causes loosely bound π-electrons in organic molecules to circulate, producing a local or induced diamagnetic field over a large spatial volume. As the molecules tumble in solution, the field generated by π-electrons in spherical substituents results in a zero net field. However, the net field generated by π-electrons in non-spherical substituents is not zero. The effect of this induced field depends on the orientation of the molecule with respect to B0,...
1.8K
Ferromagnetism
3.3K
Materials like iron, nickel, and cobalt consist of magnetic domains, within which the magnetic dipoles are arranged parallel to each other. The magnetic dipoles are rigidly aligned in the same direction within a domain by quantum mechanical coupling among the atoms. This coupling is so strong that even thermal agitation at room temperature cannot break it. The result is that each domain has a net dipole moment. However, some materials have weaker coupling, and are ferromagnetic at lower...
3.3K
Paramagnetism
3.1K
Paramagnets are materials with unpaired electrons that possess a finite magnetic moment. In the absence of a magnetic field, these moments are randomly oriented, and thus the net moment is zero. Under an external field, a torque acting on the moments tends to align them along the field's direction. However, the random thermal motion of electrons produces a torque opposite to the external field and tries to disorient the moments. These two competing effects align only a few moments along the...
3.1K
Magnetic Force
2.2K
In addition to the electric forces between electric charges, moving electric charges exert magnetic forces on each other. A magnetic field is created by a moving charge or a group of moving charges known as the electric current. A magnetic force is experienced by a second current or moving charge in response to this magnetic field. Fundamentally, interactions between moving electrons in the atoms of two bodies produce magnetic forces between them.
The magnetic force acting on a moving charge...
The magnetic force acting on a moving charge...
2.2K

