“…Here, spontaneously generated Marangoni stresses at the droplet interface lead to their propulsion . While the propulsion mechanisms mentioned above may differ among the different artificial swimmers, their characteristics remain the same: a directed ballistic motion at short time scales followed by a random motion at longer time scales. , However, the translational and rotational diffusivities depend on various parameters such as swimmer size, the magnitude of the propulsion force , and also the presence of solutes in the surrounding medium. − Microswimmer–wall effects have also been known to affect the motion characteristics significantly. − Self-propelled JCs have been studied by subjecting them to diversified environments such as externally imposed flow, − topological obstacles, , and fluid interfaces ,, or placing them in a pool of passive tracers. − Recent studies have also demonstrated tuning of the dynamics of active JCs by altering their surface morphologies. , …”