“…Active bath-mediated interactions between suspended inclusions can substantially be affected also by the presence of any confining boundaries 51 , 77 , shape, mobility and concentrations 48 , 51 , 52 , 68 , 75 , 78 and, if present, dissimilarity 49 , 69 and permeability 52 , 79 of the inclusions. On the other hand, the shape of active particles itself plays a crucial role in determining their bulk properties 37 , 80 – 83 , near-wall accumulations at rigid 40 – 43 , 56 , 84 and deformable 85 – 87 boundaries and, hence, the active (or ‘swim’) pressure they exert on these boundaries 56 , 64 , 79 , 88 , 89 , and the effective interactions they mediate between external objects 47 , 66 , 68 , 69 . For instance, the nonequilibrium wall accumulation of self-propelled rods turns out to be weaker than that of self-propelled disks 41 , 42 .…”