Related Experiment Video
Updated: Apr 25, 2026

09:06
Visualizing Uniaxial-strain Manipulation of Antiferromagnetic Domains in Fe1+YTe Using a Spin-polarized Scanning Tunneling Microscope
Published on: March 24, 2019
6.6K
Composite fermions with tunable Fermi contour anisotropy.
D Kamburov1, Yang Liu1, M Shayegan1
1Department of Electrical Engineering, Princeton University, Princeton, New Jersey 08544, USA.
Physical Review Letters
|August 29, 2014
Summary
Investigating composite fermions in two-dimensional systems reveals how parallel magnetic fields distort their Fermi contours. This finding advances understanding of quantum phenomena in low-temperature, high-field environments.
Area of Science:
- Condensed Matter Physics
- Quantum Materials
- Two-Dimensional Electron Systems
Background:
- Composite fermion (CF) theory explains complex behaviors in 2D systems under strong magnetic fields.
- CFs are quasiparticles formed by attaching flux quanta to electrons, simplifying interactions.
- At half-filled Landau levels, CFs experience zero effective magnetic field, forming a distinct Fermi surface.
Purpose of the Study:
- To investigate the impact of parallel magnetic fields on CF Fermi contours.
- To explore the distortion of the Fermi surface in a 2D hole system.
Main Methods:
- Experimental measurements on a high-quality two-dimensional hole system.
- Utilizing a GaAs quantum well structure.
- Applying strong perpendicular and parallel magnetic fields.
Main Results:
- Demonstrated significant distortion of the hole-flux composite fermion Fermi contour.
- Observed the influence of parallel magnetic fields on CF properties.
- Provided experimental evidence for theoretical predictions.
Conclusions:
- Parallel magnetic fields play a crucial role in modifying the Fermi surface of composite fermions.
- The findings offer new insights into the behavior of 2D systems in magnetic fields.
- Highlights the sensitivity of composite fermion states to magnetic field orientation.
Related Concept Videos
Fermi Level
2.5K
The Fermi-Dirac function is represented by an S-shaped curve indicating the probability of an energy state being occupied by an electron at a given temperature. The Fermi level is the energy level at which there is a fifty percent chance of finding an electron, and it is positioned between the lower-energy valence band and the higher-energy conduction band.
At absolute zero temperature, electrons fill all energy states up to the Fermi level, leaving upper states empty. As the temperature rises,...
At absolute zero temperature, electrons fill all energy states up to the Fermi level, leaving upper states empty. As the temperature rises,...
2.5K
Fermi Level Dynamics
1.1K
The vacuum level denotes the energy threshold required for an electron to escape from a material surface. It is usually positioned above the conduction band of a semiconductor and acts as a benchmark for comparing electron energies within various materials.
Electron affinity in semiconductors refers to the energy gap between the minimum of its conduction band and the vacuum level and it is a critical parameter in determining how easily a semiconductor can accept additional electrons.
The work...
Electron affinity in semiconductors refers to the energy gap between the minimum of its conduction band and the vacuum level and it is a critical parameter in determining how easily a semiconductor can accept additional electrons.
The work...
1.1K
Ferromagnetism
2.8K
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...
2.8K
Biasing of Metal-Semiconductor Junctions
903
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...
903
Valence Bond Theory
8.9K
Coordination compounds and complexes exhibit different colors, geometries, and magnetic behavior, depending on the metal atom/ion and ligands from which they are composed. In an attempt to explain the bonding and structure of coordination complexes, Linus Pauling proposed the valence bond theory, or VBT, using the concepts of hybridization and the overlapping of the atomic orbitals. According to VBT, the central metal atom or ion (Lewis acid) hybridizes to provide empty orbitals of suitable...
8.9K
Biasing of FET
1.0K
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...
In an N-channel JFET, the structure consists of N-type material forming the channel on a P-type substrate, with the...
1.0K

