Skip to main content
. 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 5.

FIGURE 5

DDM analysis reveals ballistic-like transport of particles entrained in active composites at mesoscopic spatiotemporal scales. (A) Sample image structure functions D(q,Δt) for composites with actin fractions ϕA indicated in the legend. All curves shown are evaluated at q=3.92μm1, and solid black lines are fits to the data to determine corresponding q-dependent decay times τ(q) and stretching exponents γ, as described in Methods. (B) Decay times τ(q) for each composite shown in (A). Dashed and dotted black lines show scaling τ(q)~qβ for ballistic (β=1) and diffusive (β=2) transport. (C) τ(q)×q2, normalized by τqmax×qmax2, for the data shown in (B). Horizontal dotted line and unity-sloped dashed line correspond to scaling indicative of normal diffusion (α=2/β=1) and ballistic motion (α=2/β=2). Color-coded solid lines correspond to power-law fits, with the corresponding exponents β and α shown in (E) and (F). For ϕA>0 composites, the fitting range is truncated to q>1.5μm1 where a single power-law is observed. (D) Scatter plot of 1/τ(q), a measure of the transport rate, for all measured q values for each ϕA. Color coding and gradient indicate ϕA and q, respectively, with light to dark shades of each color indicating increasing q values. (E) DDM scaling exponents β determined from fits shown in (C). (F) Anomalous scaling exponents α2 determined from τ(q) fits (filled circles, αDDM=2/β), as well as the large-Δt regime fits of the MSDs (open triangles, αMSD,2) and van Hove distributions (open triangles, αvH,2) measured via SPT (see Figures 2, 3). Error bars indicate 95% confidence intervals of fits. (G) Stretching exponent γ(q), averaged over all q values, for each composite ϕA, with error bars indicating standard error.