We use analytic and numerical methods to determine the density of states of
a one-dimensional electron gas coupled to a spatially random quasistatic b
ackscattering potential of long correlation length. Our results provide ins
ight into the ''pseudogap'' phenomenon occurring in underdoped high-T-c sup
erconductors, quasi-one-dimensional organic conductors, and liquid metals.
They demonstrate the important role played by amplitude fluctuations of the
backscattering potential and by fluctuations in gradients of the potential
, and confirm the importance of the self-consistency which is a key feature
of the "fluctuation exchange'' type approximations for the electron Green'
s function. Our results allow an assessment of the merits of different appr
oximations: a previous approximate treatment presented by Sadovskii and, we
show, justified by a WKB approximation gives a reasonably good representat
ion, except for a ''central peak'' anomaly, of our numerically computed den
sities of states, whereas a previous approximation introduced by Lee, Rice,
and Anderson is not as accurate.