In order to better understand the geometry of the polymer collapse tra
nsition, we study the distribution of geometric clusters made up of th
e nearest neighbor interactions of an interacting self-avoiding walk.
We argue for this new correlated percolation problem that in two dimen
sions, and possibly also in three dimensions, a percolation transition
takes place at a temperature lower than the collapse transition. Henc
e this novel transition should be governed by exponents unrelated to t
he theta-point exponents. This also implies that there is a temperatur
e range in which the polymer has collapsed, but has no long-range clus
ter structure. We use Monte Carlo to study the distribution of cluster
s on the simple cubic and Manhattan lattices. On the Manhattan lattice
, where the data are most convincing, we find that the percolation tra
nsition occurs at omega(p) = 1.461(3), while the collapse transition i
s known to occur exactly at omega(0) = 1.414.... We propose a finite-s
ize scaling form for the cluster distribution and estimate several of
the critical exponents. Regardless of the Value of omega(p), this perc
olation problem sheds new light on polymer collapse.