Painlevé Conjecture
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physics Physics is the scientific study of matter, its Elementary particle, fundamental constituents, its motion and behavior through space and time, and the related entities of energy and force. "Physical science is that department of knowledge whi ...
, the Painlevé conjecture is a theorem about singularities among the solutions to the ''n''-body problem: there are noncollision singularities for ''n'' ≥ 4. The theorem was proven for ''n'' ≥ 5 in 1988 by Jeff Xia and for n = 4 in 2014 by Jinxin Xue.


Background and statement

Solutions (\mathbf,\mathbf) of the ''n''-body problem \dot = M^\mathbf,\; \dot = \nabla U(\mathbf) (where M are the masses and U denotes the
gravitational potential In classical mechanics, the gravitational potential is a scalar potential associating with each point in space the work (energy transferred) per unit mass that would be needed to move an object to that point from a fixed reference point in the ...
) are said to have a singularity if there is a sequence of times t_n converging to a finite t^* where \nabla U\left(\mathbf\left(t_n\right)\right) \rightarrow \infty. That is, the forces and accelerations become infinite at some finite point in time. A ''collision singularity'' occurs if \mathbf(t) tends to a definite limit when t \rightarrow t^*, t. If the limit does not exist the singularity is called a ''pseudocollision'' or ''noncollision'' singularity.
Paul Painlevé Paul Painlevé (; 5 December 1863 – 29 October 1933) was a French mathematician and statesman. He served twice as Prime Minister of France, Prime Minister of the French Third Republic, Third Republic: 12 September – 13 November 1917 and 17 A ...
showed that for ''n'' = 3 any solution with a finite time singularity experiences a collision singularity. However, he failed at extending this result beyond 3 bodies. His 1895 Stockholm lectures end with the conjecture:


Development

Edvard Hugo von Zeipel proved in 1908 that if there is a collision singularity, then J(\mathbf(t)) tends to a definite limit as t\rightarrow t^*, where J(\mathbf)=\sum_i m_i , \mathbf_i, ^2 is the
moment of inertia The moment of inertia, otherwise known as the mass moment of inertia, angular/rotational mass, second moment of mass, or most accurately, rotational inertia, of a rigid body is defined relatively to a rotational axis. It is the ratio between ...
. This implies that a necessary condition for a noncollision singularity is that the velocity of at least one particle becomes unbounded (since the positions \mathbf remain finite up to this point). Mather and McGehee managed to prove in 1975 that a noncollision singularity can occur in the co-linear 4-body problem (that is, with all bodies on a line), but only after an infinite number of (regularized) binary collisions. Donald G. Saari proved in 1977 that for
almost all In mathematics, the term "almost all" means "all but a negligible quantity". More precisely, if X is a set (mathematics), set, "almost all elements of X" means "all elements of X but those in a negligible set, negligible subset of X". The meaning o ...
(in the sense of
Lebesgue measure In measure theory, a branch of mathematics, the Lebesgue measure, named after French mathematician Henri Lebesgue, is the standard way of assigning a measure to subsets of higher dimensional Euclidean '-spaces. For lower dimensions or , it c ...
) initial conditions in the plane or space for 2, 3 and 4-body problems there are singularity-free solutions. In 1984, Joe Gerver gave an argument for a noncollision singularity in the planar 5-body problem with no collisions. He later found a proof for the 3''n'' body case. Finally, in his 1988 doctoral dissertation, Jeff Xia demonstrated a 5-body configuration that experiences a noncollision singularity. Joe Gerver has given a heuristic model for the existence of 4-body singularities. In his 2013 doctoral thesis at University of Maryland, Jinxin Xue considered a simplified model for the planar four-body problem case of the Painlevé conjecture. Based on a model of Gerver, he proved 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 earlier collisions. In 2014, Xue extended his previous work and proved the conjecture for n=4. Due to the symmetry constraint, Xia's model is only valid for the 5-body problem. Gerver-Xue's model does not have such a constraint, and is likely to be generalized to the general N>4 body problem.


References

{{DEFAULTSORT:Painleve conjecture Gravity Orbits Classical mechanics Dynamical systems Conjectures that have been proved