Abstract
We study the dynamics of ring ferrodark solitons (FDSs) in a homogeneous quasi-two-dimensional (2D) ferromagnetic spin-1 Bose-Einstein condensate (BEC). In contrast to the usual expanding dynamics of ring dark solitons in a homogeneous system, the ring FDS radius exhibits self-sustained oscillations accompanied by the nematic tensor breathing at the magnetization-vanishing ring FDS core. When the ring radius greatly exceeds the FDS width, motion is nearly elastic, and we derive the ring-radius equation of motion (EOM) which admits exact solutions. This equation can be recast into a form analogous to the inviscid Rayleigh-Plesset equation governing spherical bubble dynamics in classical fluids, but with anomalous terms. At the ring FDS core, the nematic tensor motion is parameterized by a single parameter that connects the two types of FDSs monotonically. Beyond the hydrodynamics regime, density and spin wave emissions become significant and cause energy loss, shrinking the ring FDS radius oscillation; below a threshold, collapses occur followed by the ring FDS annihilation. In the zero quadratic Zeeman energy limit, the ring radius and eigenvalues of the nematic tensor become stationary, while oscillations of the nematic tensor components, driven by the ring curvature, persist at the core. Excellent agreements are found between analytical predictions and numerical simulations.