We discuss some aspects of the time picture of tunneling for open quan
tum systems described by non-Hermitian (NH) Hamiltonians. The concept
of sojourn time for such systems is introduced in the framework of the
biorthonormal formalism. Due to the various definitions of probabilit
y density in the non-Hermitian case, we get three different sojourn ti
mes, two real and one complex. We consider as model of a dissipative N
H system the complex, generalized parametric oscillator, for which we
derive the exact expressions of the three sojourn times in terms of th
e Wei-Norman characteristic functions entering the non-unitary evoluti
on operators. The special case of the inverted Caldirola-Kanai oscilla
tor with complex friction parameter is investigated for an initial ext
ended wavepacket. We also discuss the Landau-Zener-like transitions of
the NH parametric oscillator, i.e. the dissipative tunneling through
a dynamical barrier due to the perturbative effect of the damping.