English

On entry-exit formulas for degenerate turning point problems in planar slow-fast systems

Dynamical Systems 2025-10-06 v1

Abstract

In this paper, we study degenerate entry-exit problems associated with planar slow-fast systems having an invariant line {(x,y):y=0}\{(x,y)\,:\,y=0\} with a turning point at x=0x=0. The degeneracy stems from the fact that the slow flow has a saddle-node of even order 2n2n, nNn\in \mathbb N, at the turning point, i.e. x=x2n(1+o(1))x' = -x^{2n}(1+o(1)) for ϵ=0\epsilon=0. We are motivated by the appearance of such turning point problems (for n=1n=1) in the graphics (I21)(I_2^1) and (I41)(I_4^1), through a nilpotent saddle-node singularity at infinity, in the Dumortier-Roussarie-Rousseau program (for solving the finiteness part of Hilbert's 16th problem for quadratic polynomial systems). Our results show, under additional hypothesis, that in the case n=1n=1 there is a well-defined entry-exit relation for ϵ0\epsilon\rightarrow 0. The associated Dulac map is smooth w.r.t. (ϵ,ϵlogϵ1)(\epsilon,\epsilon \log \epsilon^{-1}). On the other hand for the cases n2n\ge 2, we show that the entry-exit relation requires additional control parameters. Our approach follows the one used by De Maesschalck, P. and Schecter, S. (JDE 2016) for a different type of degenerate entry-exit problem. In particular, we apply blow-up {after} having first performed a singular coordinate transformation of yy. The degeneracy at x=0x=0 requires an additional blow-up. We finally apply the result for n=1n=1 to a normal form for the unfolding of the \NEW{relevant} graphics in the Dumortier-Roussarie-Rousseau program. Here we also demonstrate that the singular transformation of yy due to De Maesschalck, P. and Schecter, S. (JDE 2016) has practical significance in numerical computations.

Keywords

Cite

@article{arxiv.2510.02770,
  title  = {On entry-exit formulas for degenerate turning point problems in planar slow-fast systems},
  author = {Renato Huzak and Kristian Uldall Kristiansen},
  journal= {arXiv preprint arXiv:2510.02770},
  year   = {2025}
}
R2 v1 2026-07-01T06:14:49.822Z