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. Author manuscript; available in PMC: 2014 Jun 6.
Published in final edited form as: J Phys Chem A. 2010 Aug 26;115(16):3657–3664. doi: 10.1021/jp1031493

Figure 3.

Figure 3

Rupture-force probability distributions for peptide aptamer binding to a) glass, b) polystyrene and c) carbon nanotubes. Histograms are fit to the model of Evans-Ritchie21 (dotted line), Hummer-Szabo22 (gray) and Dudko et al.23 assuming a cusp shaped (ν=1/2, black solid line) or a linear-cubic (ν=2/3, black dashed line) energy barrier.