“…As expected from dilute dispersions of randomly oriented thin discs, the scattering intensity in the middle-q range follows a power law (i.e., I(q) ∝ q −α , where α = 2). 27 The scattering curve from a 1.0 wt % Laponite−H 2 O solution without monomer, also present in Figure S5, practically overlaps with that of the 1.0 wt % solution with monomer, demonstrating the negligible contribution from the monomer to the overall SAXS signal. Three of the curves, 1.0, 1.5, and 2.0 wt %, were fitted using the form factor for thin discs 28 (eq 1), where R and 2H are the radius and thickness of the particles, respectively, J 1 (x) is the first-order Bessel function, α is the angle between the axis of the disc and the scattering vector q, (ρ e,clay − ρ e,H 2 O ) is the electron density contrast between the Laponite platelets and water, N clay is the number of clay platelets per unit volume, and v clay is the volume of a single disc.…”