Denoting by M(L) the number of cells in the largest cluster, simulations show in the limit of large L, M(L) scales as
| ln(L) | for p < pc |
| Ld | for p = pc |
| L2 | for p > pc |
where d = 1.89 +/- 0.03.
That is, at the percolation threshold, the largest cluster is a statistically self-similar fractal.
For percolation on triangular lattices, in 1964
Sykes and Essam showed analytically that
Return to percolation.