Abstract
The tunneling through a potential barrier in a Coulomb gas confined in a quantum wire is discussed. The tunneling conductance g(T) at temperature T is found to be [g(T)∝exp, \left[ln, \frac{vF}{WT}-\frac{2}{3r}, \left {\left(1+r, ln, \frac{vF}{WT}\
ight)3/2-1\
ight}\
ight], \
]where W is the width of the wire, vF is the Fermi velocity, and r=(8/π 2)rs=4e2/π vFε 0 is the dimensionless mean separation between electrons.