Laughlin Wavefunction

Fractional quantum Hall effect at filling fraction ν=1/m. The Laughlin wavefunction describes strongly correlated electrons with fractional charge e/m quasiparticle excitations.

Ψ = ∏ᵢ﹤ⱼ(zᵢ−zⱼ)ᵐ · e^{−Σ|zᵢ|²/4}
Filling fraction: ν = 1/3
Particles: 12
Quasiparticle charge: e/3