A system where electrons are confined to move in a plane, exhibiting quantum effects.A two-dimensional electron gas (2DEG) is a system in which electrons are confined to move in a single plane, typically at the interface between two different semiconductor materials. At low temperatures and in high magnetic fields, this confinement leads to striking quantum phenomena, such as the quantum Hall effect, where the electrical conductivity becomes quantized in exact integer or fractional multiples of fundamental constants. The 2DEG is a cornerstone of condensed matter physics, providing a clean experimental platform to study quantum mechanics on a macroscopic scale.
The concept emerged in the 1960s–1970s with the development of semiconductor heterostructures, and the integer quantum Hall effect was discovered by Klaus von Klitzing in 1980, followed by the fractional quantum Hall effect by Daniel Tsui, Horst Störmer, and Robert Laughlin in 1982.
The confinement is achieved by sandwiching a thin layer of a semiconductor (like gallium arsenide) between layers of a wider-bandgap material (like aluminum gallium arsenide). Electrons fall into a potential well at the interface, and their motion perpendicular to the plane is quantized into discrete energy levels. At low temperatures, only the lowest of these levels is occupied, so the electrons behave as a truly two-dimensional quantum system. In a strong magnetic field, the in-plane motion also becomes quantized, forming Landau levels, which give rise to the quantum Hall effects.
2DEGs are used in high-electron-mobility transistors (HEMTs), which are key components in high-frequency amplifiers for satellite communications and radar systems, as well as in quantum Hall resistance standards for metrology.
In a 2DEG, electrons can form a 'Wigner crystal'—a regular lattice of electrons—when the density is low enough and the temperature is near absolute zero, a state predicted by Eugene Wigner in 1934 and observed decades later.





