Torsion and semi-degeneracy of second-order maximally superintegrable systems
Jeremy Nugent, Andreas Vollmer
TL;DR
This work identifies a geometric obstruction, the tensor $N_{ijk}$, that governs whether a $(n+1)$-parameter, second-order maximally superintegrable system extends to a non-degenerate system. The authors prove that extendability is equivalent to the vanishing of $N$, and they show this condition remains valid under conformal transformations, yielding a conformal extension criterion. They reinterpret the criterion in terms of statistical manifolds with torsion, linking $N$ to vectorial torsion of a dual connection and providing a clean, covariant framework for classifying semi-degenerate versus extendable systems. The results provide both a practical test for extension and a conceptual bridge between superintegrability, Wilczynski-type equations, and torsionful geometric structures, with potential applications to higher-dimensional integrable systems and conformal variants.
Abstract
The isotropic harmonic oscillator and the Kepler-Coulomb system are pivotal models in the Sciences. They are two examples of second-order (maximally) superintegrable (Hamiltonian) systems. These systems are classified in dimension two. A partial classification exists in dimension three. In this paper, our focus is on second-order superintegrable systems with a $(n+1)$-parameter potential with $n\geq3$. We find that these systems are underpinned by an information-geometric structure, namely the structure of a statistical manifold with torsion. We obtain a necessary and sufficient condition for such systems to extend to non-degenerate systems, i.e. to admit a maximal family of compatible potentials. The condition is geometric: we show that a $(n+1)$-parameter potential is the restriction of a non-degenerate potential if and only if a certain trace-free tensor field vanishes. We interpret this condition as the requirement that a certain affine connection has vectorial torsion. We also show that the condition for a system to be extendable is conformally invariant, allowing us to extend our results to second-order conformally superintegrable systems with a $(n+1)$-parameter potential.
