We consider transport through a one-dimensional conductor subjected to
an external periodic potential acid connected to noninteracting leads
(a ''Mott quantum wire''). In the case of a strong periodic potential
, the conductance is shown to jump from zero, for the chemical potenti
al Ising within the Mott-Hubbard gap, to the noninteracting value of 2
e(2)/h, as soon as the chemical potential crosses the gap edge. This b
ehavior is strikingly different from that of optical conductivity, whi
ch varies continuously with the carrier concentration, In the case of
a weak potential, the perturbative correction to the conductance due t
o umklapp scattering is absent away from half filling. [S0031-9007(98)
05293-4].