The monomer quantification was carried out using four different methods of Taylorgram deconvolution following the reasoning that (i) the observed signal is a sum of contributions from diffusive particles (i.e., monomers) with a Gaussian distribution, and non-diffusive particles (i.e., fibrils/nanoparticles) exhibiting an asymmetrical distribution, and (ii) that the monomer concentration is proportional to the signal amplitude of the former.