The tail eigenstates, having an anomalously small real part of energy Re (e
psilon) are considered for the non-Hermitian disordered Hamiltonian with an
imaginary random potential. Unlike in the case of Hermitian quantum mechan
ics, our tail states are extended over a parametrically large region. Such
states appear if the values of the random potential accidentally happens to
be anomalously close inside the region. Analytical results for the density
of tail states are confirmed by numerical simulations.