A quasiparticle charge that is a fraction of the elementary electron charge, arising from strong correlations.Fractional charge refers to the phenomenon where a quasiparticle in a condensed-matter system carries an electric charge that is a fraction of the electron's charge, such as e/3 or e/5. This arises in strongly correlated electron systems, most famously in the fractional quantum Hall effect, where electrons in a two-dimensional layer under a strong magnetic field form a quantum fluid with excitations that carry fractional charges. This challenges the notion that electric charge is always quantized in integer multiples of the electron charge.
The fractional quantum Hall effect was discovered experimentally by Daniel Tsui and Horst Störmer in 1982, and the theoretical explanation was provided by Robert Laughlin in 1983, who introduced the concept of fractional charge. This work earned them the 1998 Nobel Prize in Physics.
In the fractional quantum Hall effect, electrons are confined to a two-dimensional plane and subjected to a strong perpendicular magnetic field. Interactions between electrons become dominant, and they form a correlated quantum state. The elementary excitations of this state are quasiparticles that carry a fraction of the electron's charge. This arises because the many-body wavefunction has a topological order, and the quasiparticles are like vortices in the quantum fluid, carrying both charge and flux in a specific ratio.
Fractional charges are a key ingredient for topological quantum computation, where quasiparticles with non-Abelian statistics (such as those in the ν=5/2 state) could be used to build fault-tolerant qubits.
The fractional charge is not a property of a single electron but of a collective excitation, and it can be directly measured in shot-noise experiments, where the current fluctuations reveal the charge of the carriers.












