English

Hyperbolic dynamics and oscillatory motions in the 3 Body Problem

Dynamical Systems 2022-08-01 v1

Abstract

Consider the planar 3 Body Problem with masses m0,m1,m2>0m_0,m_1,m_2>0. In this paper we address two fundamental questions: the existence of oscillatory motions and of chaotic hyperbolic sets. In 1922, Chazy classified the possible final motions of the three bodies, that is the behaviors the bodies may have when time tends to infinity. One of the possible behaviors are oscillatory motions, that is, solutions of the 3 Body Problem such that the positions of the bodies q0,q1,q2q_0, q_1, q_2 satisfy lim inft±supi,j=0,1,2,ijqiqj<+ and lim supt±supi,j=0,1,2,ijqiqj=+. \liminf_{t\to\pm\infty}\sup_{i,j=0,1,2, i\neq j}\|q_i-q_j\|<+\infty \quad \text{ and }\quad \limsup_{t\to\pm\infty}\sup_{i,j=0,1,2, i\neq j}\|q_i-q_j\|=+\infty. Assume that all three masses m0,m1,m2>0m_0,m_1,m_2>0 are not equal. Then, we prove that such motions exists. We also prove that one can construct solutions of the three body problem whose forward and backward final motions are of different type. This result relies on constructing invariant sets whose dynamics is conjugated to the (infinite symbols) Bernouilli shift. These sets are hyperbolic for the symplectically reduced planar 3 Body Problem. As a consequence, we obtain the existence of chaotic motions, an infinite number of periodic orbits and positive topological entropy for the 3 Body Problem.

Keywords

Cite

@article{arxiv.2207.14351,
  title  = {Hyperbolic dynamics and oscillatory motions in the 3 Body Problem},
  author = {Marcel Guardia and Pau Martín and Jaime Paradela and Tere M. Seara},
  journal= {arXiv preprint arXiv:2207.14351},
  year   = {2022}
}

Comments

107 pages

R2 v1 2026-06-25T01:19:00.170Z