Suspended colloidal particles interacting chemically with a solute can self-propel by autophoretic motion when they are asymmetrically patterned (Janus colloids). Here we demonstrate theoretically that such anisotropy is not necessary for locomotion and that the nonlinear interplay between surface osmotic flows and solute advection can produce spontaneous, and self-sustained motion of isotropic particles. Solving the classical autophoretic framework for isotropic particles, we show that, for given material properties, there exists a critical particle size (or Péclet number) above which spontaneous symmetry-breaking and autophoretic motion occur. A hierarchy of instabilities is further identified for quantized critical Péclet numbers.The locomotion of microorganisms has long been used as a motivation and a practical inspiration for the design of synthetic self-propelled particles. Typically, biological cells generate propulsion by deforming their slender appendages, termed flagella or cilia, in a non-time-reversible fashion 1 . However, and perhaps not surprisingly given the numerous microfabrication challenges, no genuinely self-propelled micro-swimmer has been manufactured in the lab so far. Instead, man-made biomimetic propellers are driven by external torques or forces. That actuation allows either to deform soft propellers whose deformed shape induce propulsion 2-4 , to continuously generate propulsion in chiral shapes 5,6 , or to exploit interactions with surfaces 7-9 .An alternative route for the production of artificial small-scale swimmers has proven to be much more successful. It consists in making miniaturized chemically powered "engines" with no moving parts, typically made of reactive Janus beads or rods 10-12 . The reaction products released by these chemically-asymmetric particles create concentration gradients which induce a net phoretic fluid motion near their surface leading to locomotion. Theoretically, the interest in these so-called autophoretic swimmers was triggered by a theoretical model which accounted for such a novel propulsion mechanism in a simple and generic fashion 13,14 . This model was then further elaborated to include the nonlinear interplay between the colloid motion and the advection of the reactants 15-17 or a more complex kinetic route for the surface chemistry 18 , to deal with the rotational Brownian motion of the swimmers 19 , and to detail the microscopic coupling between the concentration gradients and the fluid flows at small scales 20 .In order to self-propel, autophoretic swimmers are chemically patterned, and it is the asymmetries in the chemical reactions on their surfaces which are responsible for locomotion in the first place. This requirement would make it thus difficult to achieve high-throughput production. An ingenious solution to such an engineering issue was recently offered with the production of isotropic self-propelled Marangoni droplets 21 . In a mechanism akin to the one responsible for the spontaneous motion of reactive droplets surfing on fluid inter...