Abstract
We prove new variational properties of the spatial isosceles orbits in the equal-mass three-body problem and analyze their linear stabilities in both the full phase space \begin{document}$\mathbb{R}^{12}$\end{document} and a symmetric subspace Γ. We prove that each spatial isosceles orbit is an action minimizer of a two-point free boundary value problem with non-symmetric boundary settings. The spatial isosceles orbits form a one-parameter set with rotation angle θ as the parameter. This set of orbits always lies in a symmetric subspace Γ and we show that their linear stabilities in the full phase space \begin{document}$\mathbb{R}^{12}$\end{document} can be simplified to two separated sub-problems: linear stabilities in Γ and \begin{document}$(\mathbb{R}^{12} \setminus Γ) \cup \{0\}$\end{document} . By applying Roberts' symmetry reduction method, we prove that the orbits are always unstable in the full phase space \begin{document}$\mathbb{R}^{12}$\end{document} , but it is linearly stable in Γ when \begin{document}$θ ∈ [0.33π, 0.48 π] \cup [0.52 π, 0.78 π]$\end{document} .
Highlights
Recall thatQ(2) = Qstart · RF (θ) = −(a1 + a2) cos 2θ −(a1 + a2) sin 2θ 0
Introduction and main resultsIn this paper, we study the variational existence and the linear stability of spatial isosceles orbits in the equal-mass three-body problem
We show that the spatial isosceles orbit is an action minimizer of a two-point free boundary value problem in χ under non-symmetric boundary settings
Summary
Q(2) = Qstart · RF (θ) = −(a1 + a2) cos 2θ −(a1 + a2) sin 2θ 0 It follows that paths P−1 and P2 are both connected to P0 at t = 0 and t = 1 respectively. By applying the uniqueness of solution of ODE system, Lemma 3.3 imply that the connected path PPP = P−1 ∪ P0 ∪ P2 is a smooth path and so PPP is a solution of the Newtonian equations in the three-body problem. It implies that a10 = −a20 in Qstart and the minimizer P0 coincides with P0, which is the spatial isosceles orbit.
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