Abstract

We explore the weak-strong-coupling Bose-Fermi duality in a model of a single-channel integer or fractional quantum Hall edge state with a finite-range interaction. The system is described by a chiral Luttinger liquid with non-linear dispersion of bosonic and fermonic excitations. We use the bosonization, a unitary transformation, and a refermionization to map the system onto that of weakly interacting fermions at low temperature TT or weakly interacting bosons at high TT. We calculate the equilibration rate which is found to scale with temperature as T5T^5 and T14T^{14} in the high-temperature ("bosonic") and the low-temperature ("fermonic") regimes, respectively. The relaxation rate of a hot particle with the momentum kk in the fermonic regime scales as k7T7k^7T^7.

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