Continuations and Bifurcations of Relative Equilibria for the Positively Curved Three-Body Problem

The positively curved three-body problem is a natural extension of the planar Newtonian three-body problem to the sphere $$\mathbb{S}^{2}$$ . In this paper we study the extensions of the Euler and Lagrange relative equilibria ( $$RE$$ for short) on the plane to the sphere. The $$RE$$ on $$\mathbb{S}^{2}$$ are not isolated in general. They usually have one-dimensional continuation in the three-dimensional shape space. We show that there are two types of bifurcations. One is the bifurcations between Lagrange $$RE$$ and Euler $$RE$$ . Another one is between the different types of the shapes of Lagrange $$RE$$ . We prove that bifurcations between equilateral and isosceles Lagrange $$RE$$ exist for the case of equal masses, and that bifurcations between isosceles and scalene Lagrange $$RE$$ exist for the partial equal masses case.

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Publication Details

Journal
Regular and Chaotic Dynamics
Published
2024-09-05
DOI
https://doi.org/10.1134/s1560354724560028
Citations
1
Primary Topic
Quantum chaos and dynamical systems
Type
article
Field-Weighted Citation Impact
0.28
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article

Continuations and Bifurcations of Relative Equilibria for the Positively Curved Three-Body Problem

Ernesto Pérez-Chavela, Toshiaki Fujiwara
1 citations
Regular and Chaotic Dynamics
Quantum chaos and dynamical systems
0.28
article

Continuations and Bifurcations of Relative Equilibria for the Positively Curved Three-Body Problem

Ernesto Pérez-Chavela, Toshiaki Fujiwara
article en
1 citations

Abstract

The positively curved three-body problem is a natural extension of the planar Newtonian three-body problem to the sphere $$\mathbb{S}^{2}$$ . In this paper we study the extensions of the Euler and Lagrange relative equilibria ( $$RE$$ for short) on the plane to the sphere. The $$RE$$ on $$\mathbb{S}^{2}$$ are not isolated in general. They usually have one-dimensional continuation in the three-dimensional shape space. We show that there are two types of bifurcations. One is the bifurcations between Lagrange $$RE$$ and Euler $$RE$$ . Another one is between the different types of the shapes of Lagrange $$RE$$ . We prove that bifurcations between equilateral and isosceles Lagrange $$RE$$ exist for the case of equal masses, and that bifurcations between isosceles and scalene Lagrange $$RE$$ exist for the partial equal masses case.

Regular and Chaotic DynamicsVol. 29(6)
Instituto Tecnológico Autónomo de México (MX), Kitasato University (JP)
Openalex Percentile: Top 45%
Quantum chaos and dynamical systems
0.28
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