Skip to main content
. 2015 Dec 22;113(1):116–121. doi: 10.1073/pnas.1517511113

Fig. 4.

Fig. 4.

(A) KMC-predicted probability of falling to the folded state M1 before reaching the intermediate state M13 starting from the Nth cluster. (B) Three structures (M10, M20, and M31 in gray) of the transition states between the folded (red) and the intermediate (brown) states obtained from A. (C) KMC-predicted probability of falling to the trapped states M2 and M4 before reaching the intermediate state M13 starting from the Nth cluster. (D) Two structures (M37 and M47 in gray) of the transition states between the trapped (orange and blue) and intermediate (brown) states obtained from C. Because the kinetic cluster-based network can only give the clusters close to the transition states, we use the probability regime of (0.35, 0.65) and (0.45, 0.55) between the two dashed blue lines in A and C, respectively, to identify the transition state (TS).