Scaling Properties of a Hybrid Fermi-Ulam-Bouncer Model
Figure 2
(a) Phase space generated from iteration of mapping (2.8) for the control
parameters and .
(b) Behavior of the positive Lyapunov exponent of the chaotic sea for the same
control parameters used in (a). The average value obtained was where the error corresponds to the standard deviation of the
10 samples. (c) Behavior of the average energy, ,
as function of