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. 2015 Aug 31;43(20):9928–9936. doi: 10.1093/nar/gkv860

Figure 3.

Figure 3.

Schematic representation of the simplified energy landscape used in our theoretical description. The state of the folded hairpin occurs at x = 0 and the state of the unfolded hairpin at x = L. The distances between the transition state and the folded and unfolded states are denoted by x and x, respectively. By definition, we have L = x + x.