The entry-exit function and geometric singular perturbation theory

For small epsilon > 0, the system (x) over dot = epsilon, (z) over dot = h(x, z, s)z, with h(x, 0, 0) < 0 for x < 0 and h(x, 0, 0) > 0 for x > 0, admits solutions that approach the x-axis while x < 0 and are repelled from it when x > 0. The limiting attraction and repulsion points are given by the well-known entry-exit function. For h(x, z, s)z replaced by h(x, z, epsilon)z(2), we explain this phenomenon using geometric singular perturbation theory. We also show that the linear case can be reduced to the quadratic case, and we discuss the smoothness of the return map to the line z = z(0), z(0) > 0, in the limit epsilon -> 0. (C) 2016 Elsevier Inc. All rights reserved.

Publication year:2016

Keywords:Entry-exit function, Geometric singular perturbation theory, Bifurcation delay, Blow-up, Turning point, entry–exit function, geometric singular perturbation theory, bifurcation delay, blow-up, turning point

BOF-keylabel:yes

IOF-keylabel:yes

BOF-publication weight:6

CSS-citation score:3

Authors:International

Authors from:Higher Education

Accessibility:Closed