We formulate the geometrical string which has been proposed in earlier
articles on the euclidean lattice. There are two essentially distinct
cases which correspond to non-self-avoiding surfaces and to soft-self
-avoiding ones. For the last case it is possible to find such spin sys
tems with local interaction which reproduce the same surface dynamics.
In the three-dimensional case this spin system is a usual Ising ferro
magnet with additional diagonal antiferromagnetic interaction and with
specially adjusted coupling constants. In the four-dimensional case t
he spin system coincides with the gauge Ising system with an additiona
l double-plaquette interaction and also with specially tuned coupling
constants. We extend this construction to random walks and random hype
rsurfaces (membrane and p-branes) of high dimensionality. We compare t
hese spin systems with the eight-vertex model and BNNNI models.