is a Siegel disc: a simply connected Fatou component on which f(z) is analytically conjugate to a Euclidean rotation of the unit disc onto itself by an irrational rotation angle.
is a Herman ring: a double connected Fatou component (an
annulus) on which f(z) is analytically conjugate to a Euclidean rotation of a round annulus, again by an irrational rotation angle.
Julia set (white) and Fatou set (dark red/green/blue) for with in the complex plane.
The components of the map contain the attracting points that are the solutions to . This is because the map is the one to use for finding solutions to the equation by
Newton–Raphson formula. The solutions must naturally be attracting fixed points.
Dynamic plane consist of Fatou 2 superattracting period 1 basins, each has only one component.
Level curves and rays in superattractive case
Julia set with superattracting cycles (hyperbolic) in the interior ( perieod 2) and the exterior (period 1)
Herman ring
The map
and t = 0.6151732... will produce a Herman ring.[2] It is shown by
Shishikura that the degree of such map must be at least 3, as in this example.
More than one type of component
If degree d is greater than 2 then there is more than one critical point and then can be more than one type of component
Herman+Parabolic
Period 3 and 105
attracting and parabolic
period 1 and period 1
period 4 and 4 (2 attracting basins)
two period 2 basins
Transcendental case
Baker domain
In case of
transcendental functions there is another type of periodic Fatou components, called Baker domain: these are "
domains on which the iterates tend to an
essential singularity (not possible for polynomials and rational functions)"[3][4] one example of such a function is:[5]
Wandering domain
Transcendental maps may have
wandering domains: these are Fatou components that are not eventually periodic.