Classification of Fatou components

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In mathematics, Fatou components are components of the Fatou set. They were named after Pierre Fatou.

Rational case

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If f is a rational function

f=P(z)Q(z)

defined in the extended complex plane, and if it is a nonlinear function (degree > 1)

d(f)=max(deg(P),deg(Q))2,

then for a periodic component U of the Fatou set, exactly one of the following holds:

  1. U contains an attracting periodic point
  2. U is parabolic[1]
  3. U 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.
  4. U 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.

Attracting periodic point

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The components of the map f(z)=z(z31)/3z2 contain the attracting points that are the solutions to z3=1. This is because the map is the one to use for finding solutions to the equation z3=1 by Newton–Raphson formula. The solutions must naturally be attracting fixed points.

Herman ring

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The map

f(z)=e2πitz2(z4)/(14z)

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

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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

Transcendental case

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Baker domain

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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] f(z)=z1+(12z)ez

Wandering domain

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Transcendental maps may have wandering domains: these are Fatou components that are not eventually periodic.

See also

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References

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Bibliography

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