“…Thus, for 0 < a < 1, all orbits of the map converge to the unique fixed point x * = 0 independent of the value of the initial conditions, while for a = 1, all initial points of the map are fixed points. When 1 < a ≤ 2, the dynamics of the tent map switches abruptly to a chaotic regime (see Behind the chaotic behaviour of the temporal trajectory, the underlying regularity of the dynamics apparent in the banded structure of the bifurcation diagram is the signature of a property called statistical periodicity which can be observed in the density distribution of an ensemble of tent maps [2,6,7,9]. Specifically, for 2 1/2 1/(n+1) < a ≤ 2 1/2 1/n , the densities of the tent map have periodicity with period T = (n + 1) for n = 1, 2, · · · .…”