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. Author manuscript; available in PMC: 2023 Aug 4.
Published in final edited form as: Front Phys. 2022 Nov 18;10:1055441. doi: 10.3389/fphy.2022.1055441

FIGURE 3.

FIGURE 3

Asymmetric non-Gaussian van Hove distributions reveal a combination of heterogeneous subdiffusion and advective transport of particles in active composites. (A) van Hove distributions G(Δd,Δt) of particle displacements Δd=ΔxΔy, measured via SPT, for lag times Δt=0.1,0.2,0.3,0.5,1,2,3,5,10,15s denoted by the color gradient going from light to dark for increasing Δt. Each panel corresponds to a different composite demarked by their ϕA value with color-coding as in Figure 2. (B) The square of the full width at half-maximum (FWHM)2 versus lag time Δt for each composite shown in (A). Solid lines are fits to (FWHM)2~Δtαi. For ϕA>0 composites we fit short (Δt1s) and long (Δt1s) lag time regimes separately. (C) The scaling exponents α as functions of ϕA determined from the fits shown in B, where α1 (stars) and α2 (triangles) correspond to scalings for the short and long Δt regimes, respectively. The dashed horizontal line denotes scaling for normal Brownian diffusion. (D) A sample G(Δd,Δt) distribution (ϕA=0.75 at Δt=10s) showing the asymmetry about the mode value Δdpeak. We divide each distribution into a leading edge (dark grey, displacements of the same sign as Δdpeak and greater in magnitude) and the trailing edge (light grey, the remaining part of the distribution). To clearly demonstrate the asymmetry, we mirror each edge about Δdpeak using dashed lines. (E) The fractional difference of the half-width at half maximum HWHM of the trailing (−) edge from the leading (+) edge, HW=HWHMHWHM+/HWHM+ for each ϕA and Δt. Color coding and gradient indicate ϕt and Δt, respectively, as in (A). Horizontal bars through each distribution denote the mean.