Under low temperatures and high magnetic fields, quasi-one dimensional orga
nic conductor (TMTSF)(2)PF6 exhibits a series of transitions to field-induc
ed spin density wave (FISDW). Slightly above the onset of superconductivity
in (TMTSF)(2)PF6, we observe a series of intervening phases that interrupt
the sequence of FISDW that gives rise to the quantum Hall effect. These ph
ases can be identified either as negative quantum numbered FISDW states or
a puzzling arboresecent phase. Detailed study of the QHE in (TMTSF)(2)PF6 r
eveals that the transport in the FISDW phases is dominated by anomalous lon
gitudinal resistivities p(xx) and p(yy) that remain finite at low temperatu
res. While the quantization of sigma(xy) is not adversely affected at high
magnetic fields, the transport in the intermediate magnetic field remains c
omplicated. In addition, the conductivity along applied magnetic field, sig
ma(zz), cannot be easily understood in terms of three-dimensional QHE and i
s suggestive of the importance of inter-layer coupling.