While Figure depicts SBSs and DoSs averaged over 100 geometries, analysing the results for individual snapshots allows us to distinguish between electrolyte and metallic configurations along the AIMD trajectory. This analysis reveals that metallic states appear in about 40 % of all snapshots already at 3.0 MPM, with a similar fraction of metallic frames appearing also at 6.0 MPM (see SI for a further quantitative analysis of the observed bimodal distribution distinctly categorising the snapshots as metallic or non-metallic). At 8.5 MPM and above, all the configurations are metallic, evidencing a completed transition to the metallic state, in agreement with previous experimental results. Let us now return to the intermediate concentration regime of 3.0 MPM, where the system flips fast between electrolyte and metallic states. From the EMT perspective, this regime is not only interesting for simulations but also from the point of view of experimental measurables such as the electrical conductivity or the related electron mobility, which are found to be highly dependent on concentration. To probe these transport properties, we analysed 500 configurations sampled from AIMD trajec-tories in 2 fs intervals at 3.0 MPM (intermediate regime) and 11.1 MPM (metallic regime). For both tions, Figure shows the corresponding time evolutions of the simulated DoS and electron mobility (see Methods for details). Our main finding is that the average time interval between flips from an electrolyte to a metal and vice versa is only a few tens of femtoseconds, namely 39 fs at 3.0 MPM. Moreover, the flipping seems to be happening in a quasi-random fashion, i.e., without a characteristic frequency, which exhibits a relatively broad distribution of time intervals the system spends in either of the two states. In contrast, at 11.1 MPM all configurations manifest a metallic behaviour with no transition to the electrolyte states.