Aspects of establishing a quasi-stationary state during polymer chargi
ng with fast electrons (40-60 keV) of a maximum range l that is only s
lightly less (< 6 mu m) than a sample thickness are considered. It was
shown that the experimentally observed high current densities measure
d at the back electrode and proportional to the fast-electron injectio
n current are incompatible with the conventional mechanism of conducti
on of the blocking layer. A new interpretation of this phenomenon land
some related effects) in terms of induction of electron autoemission
in the sites of local enhancement of an electric field at the head of
a short track of electrons in the plane x = l followed by propagation
of primary channels (streamers) through the full depth of the blocking
layer; however, this penetration does not cause breakdown in the samp
le.