A quasiparticle in two dimensions whose exchange statistics are neither bosonic nor fermionic, enabling braiding.Anyons are quasiparticles that exist only in two-dimensional systems, where their exchange statistics are neither bosonic (symmetric) nor fermionic (antisymmetric), but can be any phase factor. This exotic behavior allows their quantum states to depend on the braiding history of the particles, making them promising for topological quantum computation.
The concept of anyons was introduced by Frank Wilczek in 1982, who coined the term to describe particles with fractional statistics in two dimensions.
In two dimensions, the path of a particle around another can be continuously deformed without crossing, so the quantum state acquires a phase that depends on the winding number. This phase can be non-trivial, meaning that exchanging two anyons changes the state by a complex factor that is not just ±1. Braiding anyons around each other performs unitary operations on the quantum state, which are topologically protected against local perturbations.
Anyons are central to topological quantum computers, where information is encoded in the braiding of anyonic quasiparticles, offering inherent error resistance.
In the fractional quantum Hall effect, electrons in a two-dimensional electron gas under a strong magnetic field form quasiparticles with fractional charge, such as e/3, which are a type of anyon.















