 ![\[fig:Rg\_xi0\] Radius of gyration normalized by the particle radius as a function of the cluster size for suspensions with $\xi=0$. Top panels are AP squirmers (a) with $r_c=0.0\sigma$ and (b) $r_c=0.0\sigma$, whereas bottom panels are WP squirmers (c) with $r_c=0.0\sigma$ and (d) $r_c=0.0\sigma$. Grey dashed lines in all panels are the function $R_g = K s^{0.00}$.](rgsxi0rc00ttganso.pdf "fig:"){width="0.00\columnwidth"}![\[fig:Rg\_xi0\] Radius of gyration normalized by the particle radius as a function of the cluster size for suspensions with $\xi=0$. Top panels are AP squirmers (a) with $r_c=0.0\sigma$ and (b) $r_c=0.0\sigma$, whereas bottom panels are WP squirmers (c) with $r_c=0.0\sigma$ and (d) $r_c=0.0\sigma$. Grey dashed lines in all panels are the function $R_g = K s^{0.00}$.](rgsxi0rc00ttganso.pdf "fig:"){width="0.00\columnwidth"} ![\[fig:Rg\_xi0\] Radius of gyration normalized by the particle radius as a function of the cluster size for suspensions with $\xi=0$. Top panels are AP squirmers (a) with $r_c=0.0\sigma$ and (b) $r_c=0.0\sigma$, whereas bottom panels are WP squirmers (c) with $r_c=0.0\sigma$ and (d) $r_c=0.0\sigma$. Grey dashed lines in all panels are the function $R_g = K s^{0.00}$.](rgsxi0rc00hhganso.pdf "fig:"){width="0.00\columnwidth"}![\[fig:Rg\_xi0\] Radius of gyration normalized by the particle radius as a function of the cluster size for suspensions with $\xi=0$. Top panels are AP squirmers (a) with $r_c=0.0\sigma$ and (b) $r_c=0.0\sigma$, whereas bottom panels are WP squirmers (c) with $r_c=0.0\sigma$ and (d) $r_c=0.0\sigma$. Grey dashed lines in all panels are the function $R_g = K s^{0.00}$.](rgsxi0rc00hhganso.pdf "fig:"){width="0.00\columnwidth"}  Fig. \[fig: