Figure 5
From: Pre-Yield Non-Affine Fluctuations and A Hidden Critical Point in Strained Crystals
The radius of gyration Rg as a function of the size nc of the droplets where we have factored out the 
, with ν = 0.64 (branched polymer) dependence. Below the percolation transition, a, the droplets for the 
and 
branches behave differently assuming string-like (ν ~ 1) and compact (ν ~ 1/2) configurations respectively. Above percolation b, the morphology of droplets changes drastically and all droplets become branched polymers.
