Non-Collision Singularities in the Planar Two-Center-Two-Body Problem
In this paper, we study a restricted four-body problem called the planar two-center-two-body problem. In the plane, we have two fixed centers Q 1 and Q 2 of masses 1, and two moving bodies Q 3 and Q 4 of masses μ ≪ 1 . They interact via Newtonian potential. Q 3 is captured by Q 2 , and Q 4 travels b...
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Published in | Communications in mathematical physics Vol. 345; no. 3; pp. 797 - 879 |
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Main Authors | , |
Format | Journal Article |
Language | English |
Published |
Berlin/Heidelberg
Springer Berlin Heidelberg
01.08.2016
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Subjects | |
Online Access | Get full text |
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Summary: | In this paper, we study a restricted four-body problem called the planar two-center-two-body problem. In the plane, we have two fixed centers
Q
1
and
Q
2
of masses 1, and two moving bodies
Q
3
and
Q
4
of masses
μ
≪
1
. They interact via Newtonian potential.
Q
3
is captured by
Q
2
, and
Q
4
travels back and forth between two centers. Based on a model of Gerver, we prove that there is a Cantor set of initial conditions that lead to solutions of the Hamiltonian system whose velocities are accelerated to infinity within finite time avoiding all earlier collisions. This problem is a simplified model for the planar four-body problem case of the Painlevé conjecture. |
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ISSN: | 0010-3616 1432-0916 |
DOI: | 10.1007/s00220-016-2688-6 |