Transition paths, the fleeting trajectories through the transition states that dominate the dynamics of biomolecular folding reactions, encapsulate the critical information about how structure forms. Owing to their brief duration, however, they have not previously been observed directly. We measured transition paths for both nucleic acid and protein folding, using optical tweezers to observe the microscopic diffusive motion of single molecules traversing energy barriers. The average transit times and the shapes of the transit-time distributions agreed well with theoretical expectations for motion over the one-dimensional energy landscapes reconstructed for the same molecules, validating the physical theory of folding reactions. These measurements provide a first look at the critical microscopic events that occur during folding, opening exciting new avenues for investigating folding phenomena.

The timescale for the microscopic dynamics of proteins during conformational transitions is set by the intrachain diffusion coefficient, D. Despite the central role of protein misfolding and aggregation in many diseases, it has proven challenging to measure D for these processes because of their heterogeneity. We used single-molecule force spectroscopy to overcome these challenges and determine D for misfolding of the prion protein PrP. Observing directly the misfolding of individual dimers into minimal aggregates, we reconstructed the energy landscape governing nonnative structure formation. Remarkably, rather than displaying multiple pathways, as typically expected for aggregation, PrP dimers were funneled into a thermodynamically stable misfolded state along a single pathway containing several intermediates, one of which blocked native folding. Using Kramers' rate theory, D was found to be 1,000-fold slower for misfolding than for native folding, reflecting local roughening of the misfolding landscape, likely due to increased internal friction. The slow diffusion also led to much longer transit times for barrier crossing, allowing transition paths to be observed directly for the first time to our knowledge. These results open a new window onto the microscopic mechanisms governing protein misfolding.intrachain diffusion | protein aggregation | prion protein | optical tweezers | single-molecule force spectroscopy T he formation of intricate 3D structures by proteins is a complex physical process. Such "folding" is typically described in terms of energy landscape theory (1) as a thermally driven diffusive search over an energy landscape in conformational space for the minimum-energy structure. In this picture, whereas the rates at which structural transitions take place are dominated by the presence of energy barriers in the landscape (2), it is the coefficient of diffusion over the landscape, D, that encapsulates the microscopic dynamics of the protein chain, setting the characteristic timescale for molecular motions. Knowledge of D provides insight into the internal friction in the protein chain as it undergoes conformational fluctuations (3) and sets the ultimate speed limit at which changes in structure can take place (4).Given the fundamental importance of the diffusion coefficient in protein folding, there has been much interest in measuring D under different conditions. Conformational diffusion has been studied extensively in peptides and unfolded proteins (5-10), using fluorescence probes such as fluorophore quenching or Förster resonant energy transfer to measure reconfiguration times. Typically, D ∼10 7 -10 8 nm 2 /s was found, although values as low as 10 5 nm 2 /s have been reported (10). Because the diffusion coefficient is inversely proportional to friction, measurements of D have been important for investigating the role and origin of internal friction along the folding pathway (6, 9). Possible links between the value of D and aggregation propensity have also been explored in intrinsically disorde...

Prion-like misfolding of superoxide dismutase 1 (SOD1) is associated with the disease ALS, but the mechanism of misfolding remains unclear, partly because misfolding is difficult to observe directly. Here we study the most misfolding-prone form of SOD1, reduced un-metallated monomers, using optical tweezers to measure unfolding and refolding of single molecules. We find that the folding is more complex than suspected, resolving numerous previously undetected intermediate states consistent with the formation of individual β-strands in the native structure. We identify a stable core of the protein that unfolds last and refolds first, and directly observe several distinct misfolded states that branch off from the native folding pathways at specific points after the formation of the stable core. Partially folded intermediates thus play a crucial role mediating between native and non-native folding. These results suggest an explanation for SOD1’s propensity for prion-like misfolding and point to possible targets for therapeutic intervention.

A zymogen-derived protein, pepsin, appears to be incapable of folding to the native state without the presence of the prosegment. To better understand the nature of the irreversible denaturation of pepsin, the present study reports on the characterization of the stability and low-resolution tertiary and secondary structures of native, alkaline unfolded and acid refolded porcine pepsin. Through a combination of small-angle neutron scattering (SANS), CD, and DSC, acid refolded pepsin (Rp) was shown to have secondary and tertiary structures intermediate between the alkaline denatured and native forms but was found to be thermodynamically stable relative to the native state. It was also observed that the acid refolded state of pepsin was dependent on the protein concentration during refolding because CD and SANS data revealed that both the secondary and tertiary structures of concentrated-refolded pepsin (>10 mg/mL) (CRp) were native-like, in contrast to the intermediate nature of Rp, refolded under dilute concentration (<10 mg/mL). Despite a native-like conformation, CRp was more stable and had substantially reduced activity compared to that of the native state, suggesting that the protein was misfolded. It is proposed that the stable but misfolded, acid-refolded states are evidence that pepsin in its native conformation was metastable. Furthermore, the disruption of the active site cleft in the denatured states could be discerned by modeling of the SANS data.