A long narrow gate across a fractional quantum Hall fluid at filling n
u=1/m with odd integer m, creates a one-dimensional (1D) system that i
s isomorphic to a disordered 1D electron gas with attractive interacti
ons. By varying the gate potential along such a line junction, it shou
ld be possible to tune through the ID localization transition, predict
ed for an attractively interacting electron gas. The key signature of
this 1D metal-insulator transition is the temperature dependence of th
e conductivity, which diverges as a power of temperature in the metall
ic phase, and vanishes rapidly in the insulator. We show that the 1D c
onductivity can be extracted from a standard Hall transport measuremen
t, in the regime where the Hall conductance is close to its quantized
value. A line junction in a nu=2/3 quantized Hall fluid is predicted t
o exhibit a similar localization transition.