We calculate the moments of transmittance, [T-n], through an open disordere
d 1D system with an imaginary vector potential, ih. It turns out that the c
ritical curves on the complex energy plane, C-n, where an exponential decay
of the appropriate quantity is changed by a power-law one, are all differe
nt. They also differ from the corresponding curves for [lnT] and that of th
e averaged one-particle Green's function; the latter defines the density of
states support for the open system. This results from the absence of self-
averaging in disordered 1D systems and reflects higher-order correlations i
n localized eigenstates of the non-Hermitian model.