Non-collision singularities exist in a planar Newtonian 4-body problem

You need to know: Euclidean plane {\mathbb R}^2, (second) derivative of a function x:{\mathbb R}\to {\mathbb R}^2.

Background: Let n point particles with masses m_i > 0 and positions x_i \in {\mathbb R}^2 are moving according to Newton’s laws of motion: m_j \frac{d^2 x_j}{dt^2} = \sum\limits_{i \neq j} \frac{m_i m_j(x_i - x j)}{r_{ij}^3}, \, 1 \leq j \leq n, where r_{ij} is the distance between x_i and x_j. The motion of particles is determined by the initial conditions: their masses and their positions and velocities at time t=0.

The Theorem: On 29th August 2014, Jinxin Xue submitted to Acta Mathematica a paper in which he proved that, for n=4, there is a non-empty set of initial conditions, such that all four points escape to infinity in a finite time, avoiding collisions.

Short context: The problem of describing motion of n bodies under gravitation (n-body problem) in space or plane is a fundamental problem in physics and mathematics, studied by many authors, see, for example, here. In general, the motion can be very complicated even for n=3, but can we at least understand under what initial conditions the solution to the system of Newton equations (presented above) is well-defined for all t\geq 0? This may be not the case for two reasons: (a) collision happened, and (b) there are no collisions but a point escape to infinity in a finite time. Case (b) is known as non-collision singularity. In 1897, Painlevé proved that there are no such singularities for n=3, but conjectured their  existence for all n>3. In 1992, Xia proved this conjecture (for motions in {\mathbb R}^3) for n\geq 5. The Theorem establishes the remaining (and the hardest) case n=4.

Links: Free arxiv version of the original paper is here, journal version is here.

Go to the list of all theorems