Abstract
The dynamics of a system defined by an endomorphism is essentially different from that of a system defined by a diffeomorphism due to interaction of invariant objects with the so-called critical locus. A planar endomorphism typically folds the phase space along curves <em>J</em><sub>0</sub> where the Jacobian of the map is zero. The critical locus is the image of <em>J</em><sub>0</sub>, denoted <em>J</em><sub>1</sub>, which is often only piecewise smooth due to the presence of cusp points that are persistent under perturbation. We investigate what happens when the stable set <em>W</em><sup>s</sup> of a fixed point or
periodic orbit interacts with <em>J</em><sub>1</sub> near such a cusp point <em>C</em><sub>1</sub>. Our approach is in the spirit of bifurcation theory and we classify the different unfoldings of the codimension-two singularity where the curve <em>W</em><sup>s</sup> is tangent to <em>J</em><sub>1</sub> exactly at <em>C</em><sub>1</sub>. The analysis uses a
local normal-form setup that identifies the possible local phase
portraits. These local phase portraits give rise to different global
manifestations of the behaviour organised by five different global
bifurcation diagrams.