A magnetic monopole in a superfluid bubble

Magnetic monopoles lie at the crossroads of gauge fields, topology, geometric phases, and charge quantization, yet they remain elusive as fundamental particles. Here we show that an emergent Dirac-monopole framework arises naturally from the dynamics of massive quantum vortices in a spherical superfluid shell. Their dynamics is formally equivalent to that of interacting charged particles constrained to a sphere in the field of a magnetic monopole. The monopole charge is fixed by the superfluid density and automatically satisfies Dirac’s quantization condition. The emergent monopole description predicts cyclotron-like vortex motion, in quantitative agreement with Gross–Pitaevskii simulations. We further show that topological frustration induced by two like-charged polar vortices gives rise to the formation of an equatorial vortex necklace, a configuration reminiscent of the polygonal cyclone clusters observed around Jupiter’s poles, before its subsequent breakup through a Kelvin–Helmholtz-like instability. Within this framework, the vortex necklace may be viewed as a quantized analogue of Wu–Yang gauge patching. Our results establish spherical superfluids as a versatile platform for realizing and exploring fundamental aspects of Dirac-monopole physics.