Periodic point#Iterated functions

{{short description|Point which a function/system returns to after some time or iterations}}

In mathematics, in the study of iterated functions and dynamical systems, a periodic point of a function is a point which the system returns to after a certain number of function iterations or a certain amount of time.

Iterated functions

Given a mapping {{mvar|f}} from a set {{mvar|X}} into itself,

:f: X \to X,

a point {{mvar|x}} in {{mvar|X}} is called periodic point if there exists an {{mvar|n}}>0 so that

:\ f_n(x) = x

where {{mvar|f{{sub|n}}}} is the {{mvar|n}}th iterate of {{mvar|f}}. The smallest positive integer {{mvar|n}} satisfying the above is called the prime period or least period of the point {{mvar|x}}. If every point in {{mvar|X}} is a periodic point with the same period {{mvar|n}}, then {{mvar|f}} is called periodic with period {{mvar|n}} (this is not to be confused with the notion of a periodic function).

If there exist distinct {{mvar|n}} and {{mvar|m}} such that

:f_n(x) = f_m(x)

then {{mvar|x}} is called a preperiodic point. All periodic points are preperiodic.

If {{mvar|f}} is a diffeomorphism of a differentiable manifold, so that the derivative f_n^\prime is defined, then one says that a periodic point is hyperbolic if

:|f_n^\prime|\ne 1,

that it is attractive if

:|f_n^\prime|< 1,

and it is repelling if

:|f_n^\prime|> 1.

If the dimension of the stable manifold of a periodic point or fixed point is zero, the point is called a source; if the dimension of its unstable manifold is zero, it is called a sink; and if both the stable and unstable manifold have nonzero dimension, it is called a saddle or saddle point.

= Examples =

A period-one point is called a fixed point.

The logistic map

x_{t+1}=rx_t(1-x_t), \qquad 0 \leq x_t \leq 1, \qquad 0 \leq r \leq 4

exhibits periodicity for various values of the parameter {{mvar|r}}. For {{mvar|r}} between 0 and 1, 0 is the sole periodic point, with period 1 (giving the sequence {{math|0, 0, 0, …,}} which attracts all orbits). For {{mvar|r}} between 1 and 3, the value 0 is still periodic but is not attracting, while the value \tfrac{r-1}{r} is an attracting periodic point of period 1. With {{mvar|r}} greater than 3 but less than {{tmath|1 + \sqrt 6,}} there are a pair of period-2 points which together form an attracting sequence, as well as the non-attracting period-1 points 0 and \tfrac{r-1}{r}. As the value of parameter {{mvar|r}} rises toward 4, there arise groups of periodic points with any positive integer for the period; for some values of {{mvar|r}} one of these repeating sequences is attracting while for others none of them are (with almost all orbits being chaotic).

Dynamical system

Given a real global dynamical system {{tmath|(\R, X, \Phi),}} with {{mvar|X}} the phase space and {{math|Φ}} the evolution function,

:\Phi: \R \times X \to X

a point {{mvar|x}} in {{mvar|X}} is called periodic with period {{mvar|T}} if

:\Phi(T, x) = x\,

The smallest positive {{mvar|T}} with this property is called prime period of the point {{mvar|x}}.

= Properties =

  • Given a periodic point {{mvar|x}} with period {{mvar|T}}, then \Phi(t,x) = \Phi(t+T,x) for all {{mvar|t}} in {{tmath|\R.}}
  • Given a periodic point {{mvar|x}} then all points on the orbit {{mvar|γ{{sub|x}}}} through {{mvar|x}} are periodic with the same prime period.

See also