FIG. 7.

(Color online) (a) Average radius of gyration 〈R_g〉∼L^v versus polymer length L. The solid line indicates the best fit to the expected power-law behavior 〈R_g〉∼L^v, obtaining v=0.75±0.07. (b) Mean-squared displacement X₂(t) versus time for different polymer lengths L=48-197. Note that X₂ grows linearly with time as expected in a diffusive process [78]. (c) By scaling the data in (b) by D∼L^α with α=0.80±0.13, we are able to collapse all the data onto a single curve. The data displayed in the plots are averages over 5000 runs 100 000-150 000 time steps long using p=0.05.