We show that the onset of the snake instability of ring dark solitons requires a broken symmetry. We also elucidate explicitly the connection between imaginary Bogoliubov modes and the snake instability, predicting the number of vortex-anti-vortex pairs produced. In addition, we propose a simple model to give a physical motivation as to why the snake instability takes place. Finally, we show that tight confinement in a toroidal potential actually enhances soliton decay due to inhibition of soliton motion.Keywords: snake instability, ring dark soliton, cylindrical symmetry, toroidal trap, ring trapThe nonlinearity of the equations of motion governing the behaviour of optical systems and ultracold atomic gases allows for interesting solutions such as bright and dark solitons [1][2][3][4], which remarkably propagate without dispersion [5] and scatter elastically. In nonlinear optics, this means that soliton light pulses sent through optical fibers propagate without changing shape, whereas in Bose-Einstein condensates and superfluid Fermi gases [6], matter wave solitons correspond to shape-maintaining dips or humps in the atomic density.In both settings dark solitons have been observed experimentally [7,8], but strictly speaking the stability holds only in one-dimensional systems. In higher dimensions, in general, they collapse into vortex-anti-vortex pairs in 2D (or vortex rings in 3D) through the snake instability [9,10], even though dark solitons retain many of their solitonic properties in nearly-integrable systems, for example, in the presence of an external trap [11]. The stability and dynamics of dark solitons has been discussed theoretically [12][13][14][15], in particular, complex frequencies in the Bogoliubov-de-Gennes (BdG) excitation spectrum have been demonstrated to drive the instability [16].Cylindrically symmetric systems, bringing forward the concepts of ring bright [17] and dark [18][19][20] solitons (RDS), offer an example of a two-dimensional system, where the dynamics can be reduced to a one-dimensional equation, and thereby making the question of stability relevant. It has been observed that filling the notch of a RDS stabilises against the snake instability [21], a result we explain in this Letter. Specifically, ring traps [22][23][24][25] might stabilise the ring dark soliton, but we show that their effect is in fact the opposite.In this Letter we consider the stability of the RDS in cylindrically symmetric confinement, showing that it is stable as long as the symmetry in the θ-direction is maintained. We show that the type of the simulation grid plays an important role related to the induced breaking of this symmetry. We propose a physical model explaining why the snake instability takes place, and further elucidate the connection between the complex BdG spectrum and the snake instability. Based on this model, we show how the number of vortex-anti-vortex pairs is directly related to the BdG spectrum.To investigate the properties of the two-dimensional condensate, we assume it is described by...