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. 2008 Sep 8;105(37):13877–13882. doi: 10.1073/pnas.0803405105

Fig. 4.

Fig. 4.

The distribution of activation barriers for the monomer (A) and dimer (B) for different regions of the folding landscape. Region I was generated from the native mMjCM and EcCM structures; region II corresponds to low energy structures obtained by the simplified model (Fig. S1); and region III corresponds to higher-energy structures from the simplified landscape (Fig. S1). The average rmsd of structures in these regions are 0.9, 3.6, and 5.3 Å, respectively. The figure presents the probability of having a given value of the activation barrier (Δg‡) as a function of the value of the activation barrier.