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...