Filled Julia set

The filled-in Julia setK(f){\displaystyle K(f)} of a polynomial f{\displaystyle f} is the union of a Julia set and its interior, non-escaping set.

Formal definition

The filled-in Julia setK(f){\displaystyle K(f)} of a polynomial f{\displaystyle f} is defined as the set of all points z{\displaystyle z} of the dynamical plane that have boundedorbit with respect to f{\displaystyle f}K(f)=def{zC:f(k)(z) as k}{\displaystyle K(f){\overset {\mathrm {def} }{{}={}}}\left\{z\in \mathbb {C} :f^{(k)}(z)\not \to \infty ~{\text{as}}~k\to \infty \right\}} where:

Relation to the Fatou set

The filled-in Julia set is the (absolute) complement of the attractive basin of infinity. K(f)=CAf(){\displaystyle K(f)=\mathbb {C} \setminus A_{f}(\infty )}

The attractive basin of infinity is one of the components of the Fatou set. Af()=F{\displaystyle A_{f}(\infty )=F_{\infty }}

In other words, the filled-in Julia set is the complement of the unbounded Fatou component: K(f)=FC.{\displaystyle K(f)=F_{\infty }^{C}.}

Relation between Julia, filled-in Julia set and attractive basin of infinity

The Julia set is the common boundary of the filled-in Julia set and the attractive basin of infinityJ(f)=K(f)=Af(){\displaystyle J(f)=\partial K(f)=\partial A_{f}(\infty )} where: Af(){\displaystyle A_{f}(\infty )} denotes the attractive basin of infinity = exterior of filled-in Julia set = set of escaping points for f{\displaystyle f}

Af() =def {zC:f(k)(z) as k}.{\displaystyle A_{f}(\infty )\ {\overset {\underset {\mathrm {def} }{}}{=}}\ \{z\in \mathbb {C} :f^{(k)}(z)\to \infty \ as\ k\to \infty \}.}

If the filled-in Julia set has no interior then the Julia set coincides with the filled-in Julia set. This happens when all the critical points of f{\displaystyle f} are pre-periodic. Such critical points are often called Misiurewicz points.

Spine

The most studied polynomials are probably those of the formf(z)=z2+c{\displaystyle f(z)=z^{2}+c}, which are often denoted by fc{\displaystyle f_{c}}, where c{\displaystyle c} is any complex number. In this case, the spine Sc{\displaystyle S_{c}} of the filled Julia set K{\displaystyle K} is defined as arc between β{\displaystyle \beta }-fixed point and β{\displaystyle -\beta }, Sc=[β,β]{\displaystyle S_{c}=\left[-\beta ,\beta \right]} with such properties:

  • spine lies inside K{\displaystyle K}.[1] This makes sense when K{\displaystyle K} is connected and full[2]
  • spine is invariant under 180 degree rotation,
  • spine is a finite topological tree,
  • Critical pointzcr=0{\displaystyle z_{cr}=0} always belongs to the spine.[3]
  • β{\displaystyle \beta }-fixed point is a landing point of external ray of angle zero R0K{\displaystyle {\mathcal {R}}_{0}^{K}},
  • β{\displaystyle -\beta } is landing point of external rayR1/2K{\displaystyle {\mathcal {R}}_{1/2}^{K}}.

Algorithms for constructing the spine:

  • detailed version is described by A. Douady[4]
  • Simplified version of algorithm:
    • connect β{\displaystyle -\beta } and β{\displaystyle \beta } within K{\displaystyle K} by an arc,
    • when K{\displaystyle K} has empty interior then arc is unique,
    • otherwise take the shortest way that contains 0{\displaystyle 0}.[5]

Curve R{\displaystyle R}: R=defR1/2ScR0{\displaystyle R{\overset {\mathrm {def} }{{}={}}}R_{1/2}\cup S_{c}\cup R_{0}} divides dynamical plane into two components.

Images

Names

Notes

References

  1. Peitgen Heinz-Otto, Richter, P.H. : The beauty of fractals: Images of Complex Dynamical Systems. Springer-Verlag 1986. ISBN 978-0-387-15851-8.
  2. Bodil Branner : Holomorphic dynamical systems in the complex plane. Department of Mathematics Technical University of Denmark, MAT-Report no. 1996-42.