"Life after death" in ordinary differential equations with a non-Lipschitz singularity
arXiv:1806.09001 · doi:10.1088/1361-6544/abbe60
Abstract
We consider a class of ordinary differential equations in -dimensions featuring a non-Lipschitz singularity at the origin. Solutions of such systems exist globally and are unique up until the first time they hit the origin, , which we term `blowup'. However, infinitely many solutions may exist for longer times. To study continuation past blowup, we introduce physically motivated regularizations: they consist of smoothing the vector field in a --ball around the origin and then removing the regularization in the limit . We show that this limit can be understood using a certain autonomous dynamical system obtained by a solution-dependent renormalization procedure. This procedure maps the pre-blowup dynamics, , to the solution ending at infinitely large renormalized time. In particular, the asymptotic behavior as is described by an attractor. The post-blowup dynamics, , is mapped to a different renormalized solution starting infinitely far in the past. Consequently, it is associated with another attractor. The -regularization establishes a relation between these two different "lives" of the renormalized system. We prove that, in some generic situations, this procedure selects a unique global solution (or a family of solutions), which does not depend on the details of the regularization. We provide concrete examples and argue that these situations are qualitatively similar to post-blowup scenarios observed in infinite-dimensional models of turbulence.
27 pages, 8 figures
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