“…Due to the low degree of functionalization and to their non-re-dispersibility after water addition (see Figure 4), dispersions 1d are lyophobic and the colloidal stability of those is provided by electrostatic repulsion. [19,[42][43][44][45] So, these dispersions can be considered as model to apply DLVO theory for carbon-based systems, [30] as has been done for fullerene dispersions made by other routes. [3,19,[44][45][46] Figure 5A presents a graphic of total interaction energy (U T ) as a function of distance for two identical spherical particles calculated based on DLVO theory, [47,48] considering the experimental radius (half of the diameters shown in Table S1) and zeta potentials for 1d dispersions, an approximate value for Hamaker constant (1 x 10 -19 J) from literature, [3] and 1:1 electrolyte (1 .…”