Research Article

On a Difference Equation with Exponentially Decreasing Nonlinearity

Figure 5

The bifurcation diagram for (2.1), with 𝛼 = 0 . 5 , 𝑝 = 2 , as 𝑞 is growing (a) and for the perturbed model (4.6) with 𝛼 = 0 . 5 , 𝑝 = 2 , a n d 𝜆 = 0 . 2 (b). We see that there is a deterministic chaos in (2.1) for 𝑞 large enough, while the perturbed model experiences chaos and then (as 𝑞 grows) the break of chaos through period-halving bifurcations.
147926.fig.005a
(a)
147926.fig.005b
(b)