On the existence of collisionless equivariant minimizers for the classical n-body problem
By D. Ferrario, S. Terracini. 2003
240 citations recorded by the source corpus.
We show that the minimization of the Lagrangian action functional on suitable classes of symmetric loops yields collisionless periodic orbits of the n-body problem, provided that some simple conditions on the symmetry group are satisfied. More precisely, we give a fairly general condition on symmetry groups G of the loop space Λ for the n-body problem (with potential of homogeneous degree -α, with α>0) which ensures that the restriction of the Lagrangian action $\mathcal{A}$ to the space ΛG of G-equivariant loops is coercive and its minimizers are collisionless, without any strong force assumption. In proving that local minima of ΛG are free of collisions we develop an averaging technique based on Marchal’s idea of replacing some of the point masses with suitable shapes (see [10]). As an application, several new orbits can be found with some appropriate choice of G. Furthermore, the result can be used to give a simplified and unitary proof of the existence of many already known minimizing periodic orbits.
Subfields: Aerospace Engineering, Astronomy and Astrophysics, Statistical and Nonlinear Physics
View Paper: https://www.semanticscholar.org/paper/c5ab19c7427b8e4df2f52338ccfab28a525b5ce3
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Citations in the corpus
- Positive periodic solutions of singular systems with a parameter (2010, background): “Periodic solutions of singular systems has been studied over many years, see, for example, [1,2,3,4,5,10,11,12,13,14,15,17] and [18,20,21,22,24,25,26,27,30].”
- Periodic solutions of second order non-autonomous singular dynamical systems (2007, background): “The question of existence of collisionless periodic orbits for Lagrangian systems with singularities has attracted much attention of many mathematicians and physicists over many years, such as [1,8,10,21,22,32].”
- Index and Stability of Symmetric Periodic Orbits in Hamiltonian Systems with Application to Figure-Eight Orbit (2009, methodology): “However in our setting the function space needs not to be a loop space, and it can be a path space, which is different from [ FT ].”