lattice model of random surfaces is studied including configurations w
ith arbitrary topologies, overhangs and bubbles. The Hamiltonian of th
e surface includes a term proportional to its area and a scale-invaria
nt integral of the squared mean curvature. We propose a discretization
of the curvature which ensures the scale-invariance of the bending en
ergy on the lattice. Nonperturbative renormalization groups for the su
rface tension and the bending rigidity are applied, which are also val
id at high temperatures and scales above the persistence length. We fi
nd at vanishing surface tensions a closed expression for the scale dep
endent rigidity including the usual logarithmic decay at low temperatu
res. Different scaling behaviours at non-vanishing tensions occur yiel
ding characteristic length scales, which determine the structure of ho
mogeneous droplet, lamellar, and microemulsion phases.