A mapping between fractional quantum Hall (FQH) junctions and the two-chann
el Kondo model is presented. We discuss this relation in detail for the par
ticular case of a junction of a FQH state at nu= 1/3 and a normal metal. We
show that in the strong coupling regime this junction has a non-Fermi-liqu
id fixed point. At this fixed point the electron Green's function has a bra
nch cut and the impurity entropy is equal to S = 1/2 In 2. We construct the
space of perturbations at the strong coupling fixed point and find that th
e dimension of the tunneling operator is 1/2. These properties are strongly
reminiscent of the non-Fermi-liquid fixed points of a number of quantum im
purity models, particularly the two-channel Kondo model. However we have fo
und that, in spite of these similarities, the Hilbert spaces of these two s
ystems are quite different. In particular, although in a special limit the
Hamiltonians of both systems are the same, their Hilbert spaces are not Sin
ce they are determined by physically distinct boundary conditions. As a con
sequence the spectrum of operators in the two problems is different.