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Map System's Orbit 📂Dynamics

Map System's Orbit

Definition1

Let the smallest natural number satisfying fk(p)=pf^{k} (p) = p for maps f:XXf : X \to X and pXp \in X be kNk \in \mathbb{N}.

  1. For map f:XXf : X \to X and point xXx \in X, the set {x,f(x),f2,}\left\{ x , f(x) , f^{2} , \cdots \right\} under ff is called the orbit of xx. Here, xx is called the initial value of the orbit.
  2. An orbit {p,f(p),f2(p),}\left\{ p , f (p) , f^{2} (p) , \cdots \right\} with the initial value pp is called a Periodic-kk Orbit, and pp is called a Periodic-kk Point.
  3. If pp is a sink of fkf^{k}, then its Periodic-kk Orbit is called a (Periodic) Sink, and if it’s a source of fkf^{k}, its Periodic-kk Orbit is called a (Periodic) Source.
  4. If for some NNN \in \mathbb{N} and all nNn \ge N, fn+k(p)=fn(p)f^{n+k} (p) = f^{n} (p) is satisfied, then pp is said to be Eventually Periodic.
  5. If there exists a periodic orbit {x1,,xn}\left\{ x_{1} , \cdots , x_{n} \right\} satisfying limnfn(p)xn=0\displaystyle \lim_{n \to \infty} | f^{n} (p) - x_{n} | = 0 for orbit {p,f(p),f2(p),,fn(p),}\left\{ p , f (p) , f^{2} (p) , \cdots , f^{n} (p) , \cdots \right\}, then {p,f(p),f2(p),,fn(p),}\left\{ p , f (p) , f^{2} (p) , \cdots , f^{n} (p) , \cdots \right\} is said to be Asymptotically Periodic.

Explanation

The existence of a Periodic-kk Orbit essentially means that fkf^{k} has a fixed point. Thus, having a cycle or a fixed point simply becomes a matter of how many times the map is applied. Therefore, after conceptual study, all theorems and higher concepts are aligned to express based on the fixed point. Let’s consider ‘period’ as a generalization of ‘fixed point’ for natural numbers.

An orbit becoming exactly like its {x1,,xn}\left\{ x_{1} , \cdots , x_{n} \right\} while being Asymptotically Periodic can also be considered Eventually Periodic. Moreover, an orbit converging to a Periodic Sink orbit is Asymptotically Periodic.

Meanwhile, for X=RX = \mathbb{R}, one can consider the following simple theorem.

Theorem2

Let us call the Periodic-kk Orbit of ff as {p1,p2,,pk}\left\{ p_{1} , p_{2} , \cdots , p_{k} \right\}.

If f(p1)f(pk)<1\left| f '(p_{1}) \cdots f '(p_{k}) \right| < 1, then {p1,p2,,pk}\left\{ p_{1} , p_{2} , \cdots , p_{k} \right\} is a sink, and if f(p1)f(pk)>1\left| f '(p_{1}) \cdots f '(p_{k}) \right| > 1, {p1,p2,,pk}\left\{ p_{1} , p_{2} , \cdots , p_{k} \right\} is a source.

Proof

By the chain rule,

(fk)(p1)=(f(fk1))(p1)=f((fk1))(fk1)(p1)=f((fk1))f((fk2))f(p1)=f(pk)f(pk1)f(p1) \begin{align*} ( f^{k} )' ( p_{1} ) =& \left( f \left( f^{k-1} \right) \right)' ( p_{1} ) \\ =& f ' \left( \left( f^{k-1} \right) \right) \left( f^{k-1} \right)' ( p_{1} ) \\ =& f ' \left( \left( f^{k-1} \right) \right) f ' \left( \left( f^{k-2} \right) \right) \cdots f ' ( p_{1} ) \\ =& f ' ( p_{k} ) f ' ( p_{k-1} ) \cdots f ' ( p_{1} ) \end{align*}

For a smooth f:RRf : \mathbb{R} \to \mathbb{R}, let’s say some pRp \in \mathbb{R} is a fixed point.

[1] If f(p)<1| f ' (p) | < 1, then pp is a sink.

[2] If f(p)>1| f ' (p) | > 1, then pp is a source.

Applying The Criterion for Sinks and Sources in 1-Dimensional Maps to (fk)(p1)=f(pk)f(pk1)f(p1)| ( f^{k} )' ( p_{1} ) | = | f ' ( p_{k} ) f ' ( p_{k-1} ) \cdots f ' ( p_{1} ) | yields the desired result.


  1. Yorke. (1996). CHAOS: An Introduction to Dynamical Systems: p13, 108. ↩︎

  2. Yorke. (1996). CHAOS: An Introduction to Dynamical Systems: p10. ↩︎