2012
DOI: 10.1137/100810381
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Existence of a Center Manifold in a Practical Domain around $L_1$ in the Restricted Three-Body Problem

Abstract: We give a proof of existence of centre manifolds within large domains for systems with an integral of motion. The proof is based on a combination of topological tools, normal forms and rigorous-computer-assisted computations. We apply our method to obtain an explicit region in which we prove existence of a center manifold in the planar Restricted Three Body Problem.

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Cited by 37 publications
(31 citation statements)
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“…These computations can be made mathematically rigorous and play a critical role in the computer assisted proof of the existence of the Lorenz attractor [77,78,79]. See also [86] for an application of mathematically rigorous computation for invariant manifolds in celestial mechanics based on normal forms. Normal forms are also useful for computing invariant tori, and are used in the numerical study of many problems coming from celestial mechanics [28,5,38,84,85].…”
Section: Related Workmentioning
confidence: 99%
“…These computations can be made mathematically rigorous and play a critical role in the computer assisted proof of the existence of the Lorenz attractor [77,78,79]. See also [86] for an application of mathematically rigorous computation for invariant manifolds in celestial mechanics based on normal forms. Normal forms are also useful for computing invariant tori, and are used in the numerical study of many problems coming from celestial mechanics [28,5,38,84,85].…”
Section: Related Workmentioning
confidence: 99%
“…We refer to the work of [18,20,21,19,36,69] for a general theory of validated computation for stable/unstable (and other types of normally hyperbolic) invariant manifolds based on the topological notion of covering relations and cone conditions. The computer assisted topological arguments are carried out in phase space using polygonal elements.…”
Section: Computing Invariant Manifolds: a Brief Overviewmentioning
confidence: 99%
“…Using the above method it is impossible to continue with the orbits to L 2 . At the fixed point one would need to apply alternative methods, such as the method of majorants [21], the Lyapunov theorem by tracing the radius of convergence of the normal form [20], or topological computer assisted tools such as those in [8,10].…”
Section: Notationmentioning
confidence: 99%