Intermittent chaos in population dynamics.

Abstract excerpt

In modelling single species with discrete, non-overlapping generations, one usually assumes that the density at time t + .1 is a function of the density at time t: Nt+1 = f(Nt). The dynamical behaviour of this system depends on the parameters in the function f. It commonly changes, as a parameter increases, from a stable equilibrium through a series of bifurcations into stable cycles, to chaotic motion. It is...

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