We study a process of anomalous diffusion of a variable resulting from
the fluctuations of a dichotomous velocity whose two states, in the a
bsence of perturbation, have the same waiting time distribution psi(t)
. In the long-time limit the function psi(t) is proportional to t(-mu)
with 2<mu<3. Previously this distribution along with the constraint o
n mu proved to be a dynamical realization of an alpha-stable Levy proc
ess with alpha=mu-1. Here we study the response of this anomalous diff
usion process to a perturbation which has the effect of truncating the
inverse power law of one of the two states of the velocity for times
t>1/epsilon, where epsilon is proportional to the intensity of the wea
k perturbation. We show that the resulting transport process is charac
terized by a succession of two regimes: the first still satisfies the
prescriptions of the Green-Kubo approach to conductivity, and, in acco
rdance with the nature of the anomalous diffusion studied here, corres
ponds to a state of increasing conductivity (IC); the second regime is
characterized by a constant conductivity (CC). The transition from th
e IC to the CC regime takes place in a time of the order of t similar
to 1/epsilon and consequently the transition occurs at longer and long
er times, as the perturbation intensity decreases. The final stationar
y regime corresponds to an asymmetric Levy process of diffusion.