Structural characteristics for the 20-mer aggregates as a function of temperature below the melting point.

Temperatures above 280.1 K are not displayed here since they are populated essentially by conformations with random coil monomers with no secondary structure. The percentages are calculated over all the structures obtained in the last 200 ns of both OPEP REMD simulations. For details on (a)–(e), see Table 2.