Structure and nature of the finite-cycle weak stability boundary Wn

Determine the dynamical and topological structure of the nth weak stability boundary Wn about the secondary body P2 in the planar circular restricted three-body problem for finite n≥1, including whether Wn is fractal and whether initial conditions on Wn lead to chaotic trajectories.

Background

The weak stability boundary Wn separates n-stable from n-unstable cycling motion about the secondary body and is central to the capture mechanism described. Earlier work suggested fractal features, but rigorous results in B24 address only the infinite-cycle limit W' and not the finite-n case.

The authors explicitly note that the structure of Wn has been an open problem and mention conjectures about fractal and chaotic behavior associated with Wn.

References

The structure of Wn about P2 has been an open problem. It was conjectured to be fractal in nature ([18]) (GG07 for brevity) and also to give rise to chaotic motion for any trajectories taking initial values on it.

Permanent Capture into the Solar System  (2407.09560 - Belbruno et al., 2024) in Section 1 (Introduction)