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.
Given a mapping from a set into itself,
f:X\toX,
fn(x)=x
If there exist distinct and such that
fn(x)=fm(x)
\prime | |
f | |
n |
\prime|\ne | |
|f | |
n |
1,
that it is attractive if
\prime|< | |
|f | |
n |
1,
and it is repelling if
\prime|> | |
|f | |
n |
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.
A period-one point is called a fixed point.
exhibits periodicity for various values of the parameter . For between 0 and 1, 0 is the sole periodic point, with period 1 (giving the sequence which attracts all orbits). For between 1 and 3, the value 0 is still periodic but is not attracting, while the value
\tfrac{r-1}{r}
\tfrac{r-1}{r}.
Given a real global dynamical system with the phase space and the evolution function,
\Phi:\R x X\toX
\Phi(T,x)=x
\Phi(t,x)=\Phi(t+T,x)