The EMC effect is studied in the perturbative QCD hard pomeron approac
h. In this framework the nuclear structure function can be expressed d
irectly in terms of the proton one. In the limit x --> 0 and for a nuc
leus with a constant density the effect is found to be a function of a
single variable which combines its x-, Q- and A-dependence. The EMC r
atio of the nuclear to nucleon structure functions goes to zero for x
--> 0 or/and A much greater than 1. At large Q(2) the effect dies out
as ln Q/Q. To describe the present data at 0.005 < x < 0.05 an attempt
is made to take into account subasymptotic effects by introducing an
anomalous dimension falling with x. This leads to a weaker x- and Q-de
pendence, which almost disappears as x grows and the anomalous dimensi
on becomes small.