The low-temperature driven or thermally activated motion of several condens
ed matter systems is often modeled by the dynamics of interfaces (co-dimens
ion-l elastic manifolds) subject to a random potential. Two characteristic
quantitative features of the energy landscape of such a many-degree-of-free
dom system are the ground-state energy and the magnitude of the energy barr
iers between given configurations. While the numerical determination of the
former can be accomplished in time polynomial in the system size, it is sh
own here that the problem of determining the latter quantity is nondetermin
istic polynomial time complete. Exact computation of barriers is therefore
(almost certainly) much more difficult than determining the exact ground st
ates of interfaces. [S1063-651X(98)14611-1].