Period-doubling bifurcation

Period-doubling bifurcation

In mathematics, a Period doubling bifurcation in a dynamical system is a bifurcation in which the system switches to a new behavior with twice the period of the original system. The hallmark of this is a Floquet multiplier of -1.

Example

Consider the following logistical map for a modified Phillips curve:

pi_{t} = f(u_{t}) + a pi_{t}^e
pi_{t+1} = pi_{t}^e + c (pi_{t} - pi_{t}^e)
f(u) = eta_{1} + eta_{2} e^{-u} ,
b > 0, 0 leq c leq 1, frac {df} {du} < 0

where pi is the actual inflation, pi^e is the expected inflation, u is the level of unemployment, and m - pi is the money supply growth rate. Keeping eta_{1} = -2.5, eta_{2} = 20, c = 0.75 and varying b, the system undergoes period doubling bifurcations, and after a point becomes chaotic, as illustrated in the bifurcation diagram on the right.

Period-halving bifurcation

A Period halving bifurcation in a dynamical system is a bifurcation in which the system switches to a new behavior with half the period of the original system. A series of period-halving bifurcations leads the system from chaos to order.

ee also

*Feigenbaum constants

External links

* [http://www.egwald.com/nonlineardynamics/onedimensionaldynamics_1.php#flipbifurcationconditions The Flip (Period Doubling) Bifurcation] in Discrete Time, Dynamic Processes


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