Non-collision singularities in a planar two-center-two-body problem

dc.contributor.advisorDolgopyat, Dmitryen_US
dc.contributor.advisorKaloshin, Vadimen_US
dc.contributor.authorXue, Jinxinen_US
dc.contributor.departmentMathematicsen_US
dc.contributor.publisherDigital Repository at the University of Marylanden_US
dc.contributor.publisherUniversity of Maryland (College Park, Md.)en_US
dc.date.accessioned2013-06-28T06:11:29Z
dc.date.available2013-06-28T06:11:29Z
dc.date.issued2013en_US
dc.description.abstractIn this work, we study a model of simplified four-body problem called planar two-center-two-body problem. In the plane, we have two fixed centers $Q_1=(-\chi,0), Q_2=(0,0)$ of masses $1$, and two moving bodies $Q_3$ and $Q_4$ of masses $\mu\ll 1$. 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 which lead to solutions of the Hamiltonian system whose velocities are accelerated to infinity within finite time avoiding all early collisions. We consider this model as a simplified model for the planar four-body problem case of the Painlev\'{e} conjecture.en_US
dc.identifier.urihttp://hdl.handle.net/1903/14043
dc.subject.pqcontrolledMathematicsen_US
dc.titleNon-collision singularities in a planar two-center-two-body problemen_US
dc.typeDissertationen_US

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