String theory in four dimensions has the unique feature that a topolog
ical term, the oriented self-intersection number, can be added to the
usual action. It has been suggested that the corresponding theory of r
andom surfaces would be free from the problem encountered in the scali
ng of the string tension. Unfortunately, in the usual dynamical triang
ulation it is not clear how to write such a term. We show that for ran
dom surfaces on a hypercubic lattice however, the analogue of the orie
nted self-intersection number I[sigma] can be defined and computed in
a straightforward way. Furthermore, I[sigma] has a genuine topological
meaning in the sense that it is invariant under the discrete analogue
of continuous deformations. The resulting random surface model is no
longer free and may lead to a non-trivial continuum limit.