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[78]). In these experiments, the triplet state of a chromophore at one peptide end is quenched upon contact formation with a chromophore attached to the opposite end of a flexible peptide. This probe of contact formation dynamics is strongly analogous to the radical recombination upon contact formation investigated here. In contrast to the observed extremely nonexponential radical recombination, however, exponential triplet decays (on the nanosecond timescale) were found in all cases. These different results can be explained by the different initial peptide conformations encountered in the two sets of experiments. In the triplet transfer experiments, the variety of peptide conformations at the moment of excitation corresponds to the equilibrium distribution, and contact formation is achieved by equilibrium fluctuations with a time-independent probability. In the radical recombination experiments, on the other hand, immediately after disulfide bond photolysis, all peptides are in conformations with small end-to-end distances: i.e., the distribution is far from equilibrium. Relaxation towards equilibrium results in a fast increase of the mean end-to-end distance and so the probability of contact formation decreases with time, as discussed in the text. For the triplet transfer experiments, moreover, peptides without internal structure were used, avoiding any internal peptide process apart from polypeptide chain diffusion. For the peptides used in the disulfide photolysis study, in contrast, additional processes such as α-helix nucleation and growth are expected to contribute to the internal peptide dynamics on longer timescales.
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