How do proteins fold so quickly? Some denatured proteins fold to their native structures in only microseconds, on average, implying that there is a folding "mechanism," i.e., a particular set of events by which the protein short-circuits a broader conformational search. Predicting protein structures using atomically detailed physical models is currently challenging. The most definitive proof of a putative folding mechanism would be whether it speeds up protein structure prediction in physical models. In the zipping and assembly (ZA) mechanism, local structuring happens first at independent sites along the chain, then those structures either grow (zip) or coalescence (assemble) with other structures. Here, we apply the ZA search mechanism to protein native structure prediction by using the AMBER96 force field with a generalized Born/surface area implicit solvent model and sampling by replica exchange molecular dynamics. Starting from open denatured conformations, our algorithm, called the ZA method, converges to an average of 2.2 Å from the Protein Data Bank native structures of eight of nine proteins that we tested, which ranged from 25 to 73 aa in length. In addition, experimental ⌽ values, where available on these proteins, are consistent with the predicted routes. We conclude that ZA is a viable model for how proteins physically fold. The present work also shows that physicsbased force fields are quite good and that physics-based protein structure prediction may be practical, at least for some small proteins.protein structure prediction ͉ replica-exchange molecular dynamics T here are two protein folding problems: one is physical and one computational. The physical problem is a puzzle about how proteins fold so quickly. In test-tube refolding experiments, protein molecules begin in a disordered denatured state (a broad ensemble of microscopic conformations) and then fold when native conditions are restored. On the one hand, folding must be stochastic: a protein's native structure is reached via many different microscopic trajectories from the broad ensemble of different starting denatured conformations. On the other hand, folding happens quickly, sometimes averaging only microseconds to reach the ordered native conformation (1). How does the process of searching and sorting through the protein's large conformational space of disordered states happen so rapidly? And how is the same native state reached from so many different starting conformations? This puzzle has been called ''Levinthal's Paradox'' (2). Even the simplest disorderto-order transitions, like the crystallization of sodium chloride, take days. It follows that the conformational search, although stochastic, cannot be random.The second folding problem is computational: predicting a protein's native structure from its amino acid sequence. Success in this area could lead to advances in computer-based drug discovery.