We then applied the trained model to predict the energy levels of all PEDOT molecules in the MD calculations throughout the entire trajectory (4 sorbitol concentrations, 8 boxes at each concentration, 64 PEDOT oligomers and 500 snapshots per box, in total 1,024,000 PEDOT molecules). The results for the pure PEDOT:PSS morphologies are shown in Figure . We find that the total disorder agrees well with the disorder predicted for only one snapshot. Analysis of the trajectories of each of the 512 PEDOT molecules allows us to extract the dynamic disorder, which surprisingly accounts for a large fraction of the total disorder. A time-average of all trajectories eventually leads to the static disorder (see Figure and). The dynamic disorder is almost independent of the sorbitol concentration (59 meV, 59 meV, 58 meV and 58 meV for 0%, 10%, 20% and 40% sorbitol concentration, respectively), while the total disorder decreases with increasing sorbitol concentration (72 meV, 67 meV, 65 meV and 64 meV). Consequently, the static disorder decreases from 42 meV at 0% sorbitol concentration to 32 meV, 27 meV and 28 meV at 10%, 20% and 40% sorbitol concentration. These disorder values are exceptionally low compared to other amorphous organic semiconductors, which is in good agreement with the high hole conductivity of PEDOT:PSS. A low static disorder increases the hopping rates which exponentially depend on the energy differences between neighboring molecules. Strong temporal fluctuations at the same time enhance the hopping attempt frequency.