• Source: Classification of Fatou components
  • In mathematics, Fatou components are components of the Fatou set. They were named after Pierre Fatou.


    Rational case


    If f is a rational function




    f
    =



    P
    (
    z
    )


    Q
    (
    z
    )





    {\displaystyle f={\frac {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
    ,


    {\displaystyle d(f)=\max(\deg(P),\,\deg(Q))\geq 2,}


    then for a periodic component



    U


    {\displaystyle U}

    of the Fatou set, exactly one of the following holds:




    U


    {\displaystyle U}

    contains an attracting periodic point




    U


    {\displaystyle U}

    is parabolic




    U


    {\displaystyle 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.




    U


    {\displaystyle 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

    =
    The components of the map



    f
    (
    z
    )
    =
    z

    (

    z

    3



    1
    )

    /

    3

    z

    2




    {\displaystyle f(z)=z-(z^{3}-1)/3z^{2}}

    contain the attracting points that are the solutions to




    z

    3


    =
    1


    {\displaystyle z^{3}=1}

    . This is because the map is the one to use for finding solutions to the equation




    z

    3


    =
    1


    {\displaystyle z^{3}=1}

    by Newton–Raphson formula. The solutions must naturally be attracting fixed points.















    = Herman ring

    =
    The map




    f
    (
    z
    )
    =

    e

    2
    π
    i
    t



    z

    2


    (
    z

    4
    )

    /

    (
    1

    4
    z
    )


    {\displaystyle f(z)=e^{2\pi it}z^{2}(z-4)/(1-4z)}


    and t = 0.6151732... will produce a Herman ring. 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



























    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)" one example of such a function is:




    f
    (
    z
    )
    =
    z

    1
    +
    (
    1

    2
    z
    )

    e

    z




    {\displaystyle f(z)=z-1+(1-2z)e^{z}}



    = Wandering domain

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


    See also


    No-wandering-domain theorem
    Montel's theorem
    John Domains
    Basins of attraction


    References


    Lennart Carleson and Theodore W. Gamelin, Complex Dynamics, Springer 1993.
    Alan F. Beardon Iteration of Rational Functions, Springer 1991.

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