  In low temperature limit, we study electron counting statistics of a
disordered conductor. We derive an expression for the distribution of charge
transmitted over a finite time interval by using a result from the random
matrix theory of quasi one dimensional disordered conductors. In the metallic
regime, we find that the peak of the distribution is Gaussian and shows
negligible sample to sample variations. We also find that the tails of the
distribution are neither Gaussian nor Poisson and exhibit strong sample to
sample variations.
