Douady rabbit explained

c

is near the center of one of the period three bulbs of the Mandelbrot set for a complex quadratic map. It is named after French mathematician Adrien Douady.

Background

zn+1

2+c
=z
n
on the complex plane, where parameter

c

is fixed to lie in one of the two period three bulb off the main cardioid and

z

ranging over the plane. The resulting image can be colored by corresponding each pixel with a starting value

z0

and calculating the amount of iterations required before the value of

zn

escapes a bounded region, after which it will diverge toward infinity.

It can also be described using the logistic map form of the complex quadratic map, specifically

zn+1=lMzn:=\gammazn\left(1-zn\right).

which is equivalent to

wn+1

2+c
=w
n
.

Irrespective of the specific iteration used, the filled Julia set associated with a given value of

\gamma

(or

\mu

) consists of all starting points

z0

(or

w0

) for which the iteration remains bounded. Then, the Mandelbrot set consists of those values of

\gamma

(or

\mu

) for which the associated filled Julia set is connected. The Mandelbrot set can be viewed with respect to either

\gamma

or

\mu

.

Noting that

\mu

is invariant under the substitution

\gamma\to2-\gamma

, the Mandelbrot set with respect to

\gamma

has additional horizontal symmetry. Since

z

and

w

are affine transformations of one another, or more specifically a similarity transformation, consisting of only scaling, rotation and translation, the filled Julia sets look similar for either form of the iteration given above.

Detailed description

You can also describe the Douady rabbit utilising the Mandelbrot set with respect to

\gamma

as shown in the graph above. In this figure, the Mandelbrot set superficially appears as two back-to-back unit disks with sprouts or buds, such as the sprouts at the one- and five-o'clock positions on the right disk or the sprouts at the seven- and eleven-o'clock positions on the left disk. When

\gamma

is within one of these four sprouts, the associated filled Julia set in the mapping plane is said to be a Douady rabbit. For these values of

\gamma

, it can be shown that

lM

has

z=0

and one other point as unstable (repelling) fixed points, and

z=infty

as an attracting fixed point. Moreover, the map

{l{M}}3

has three attracting fixed points. A Douady rabbit consists of the three attracting fixed points

z1

,

z2

, and

z3

and their basins of attraction.

For example, Figure 4 shows the Douady rabbit in the

z

plane when

\gamma=\gammaD=2.55268-0.959456i

, a point in the five-o'clock sprout of the right disk. For this value of

\gamma

, the map

lM

has the repelling fixed points

z=0

and

z=.656747-.129015i

. The three attracting fixed points of

{lM}3

(also called period-three fixed points) have the locations

\begin{align} z1&=0.499997032420304-(1.221880225696050 x 10-6)i{}{}{(red)

},\\z_2 &= 0.638169999974373 - (0.239864000011495)i,\\z_3 &= 0.799901291393262 - (0.107547238170383)i.\end

The red, green, and yellow points lie in the basins

B(z1)

,

B(z2)

, and

B(z3)

of

{lM}3

, respectively. The white points lie in the basin

B(infty)

of

lM

.

The action of

lM

on these fixed points is given by the relations

{lM}z1=z2

,

{lM}z2=z3

, and

{lM}z3=z1

.

Corresponding to these relations there are the results

\begin{align} {lM}B(z1)&=B(z2){}{or

} \subseteq,\\B(z_2)&=B(z_3) \subseteq,\\B(z_3)&=B(z_1) \subseteq.\end

As a second example, Figure 5 shows a Douady rabbit when

\gamma=2-\gammaD=-.55268+.959456i

, a point in the eleven-o'clock sprout on the left disk (

\mu

is invariant under this transformation). This rabbit is more symmetrical in the plane. The period-three fixed points then are located at

\begin{align} z1&=0.500003730675024+(6.968273875812428 x 10-6)i{}{}({red

}),\\z_2&=-0.138169999969259 + (0.239864000061970)i,\\z_3&= -0.238618870661709 - (0.264884797354373)i .\end

The repelling fixed points of

lM

itself are located at

z=0

and

z=1.450795+0.7825835i

. The three major lobes on the left, which contain the period-three fixed points

z1

,

z2

, and

z3

, meet at the fixed point

z=0

, and their counterparts on the right meet at the point

z=1

. It can be shown that the effect of

lM

on points near the origin consists of a counterclockwise rotation about the origin of

\arg(\gamma)

, or very nearly

120\circ

, followed by scaling (dilation) by a factor of

|\gamma|=1.1072538

.

Variants

A twisted rabbit[1] is the composition of a rabbit polynomial with

n

powers of Dehn twists about its ears.[2]

The corabbit is the symmetrical image of the rabbit. Here parameter

c-0.1226-0.7449i

. It is one of 2 other polynomials inducing the same permutation of their post-critical set are the rabbit.

3D

The Julia set has no direct analog in three dimensions.

4D

A quaternion Julia set with parameters

c=-0.123+0.745i

and a cross-section in the

xy

plane. The Douady rabbit is visible in the cross-section.

Embedded

A small embedded homeomorphic copy of rabbit in the center of a Julia set[3]

Fat

The fat rabbit or chubby rabbit has c at the root of the 1/3-limb of the Mandelbrot set. It has a parabolic fixed point with 3 petals.[4]

n-th eared

In general, the rabbit for the

period-(n+1)

th bulb of the main cardioid will have

n

ears[5] For example, a period four bulb rabbit has three ears.

Perturbed

Perturbed rabbit[6]

Twisted rabbit problem

In the early 1980s, Hubbard posed the so-called twisted rabbit problem, a polynomial classification problem. The goal is to determine Thurston equivalence types of functions of complex numbers that usually are not given by a formula (these are called topological polynomials):[7]

The problem was originally solved by Laurent Bartholdi and Volodymyr Nekrashevych[8] using iterated monodromic groups. The generalization of the problem to the case where the number of post-critical points is arbitrarily large has been solved as well.[9]

See also

References

  1. Web site: A Geometric Solution to the Twisted Rabbit Problem by Jim Belk, University of St Andrews . 2022-05-03 . 2022-11-01 . https://web.archive.org/web/20221101023328/https://e.math.cornell.edu/people/belk/talkslides/TwistedRabbitTalkMichigan.pdf . live.
  2. Laurent Bartholdi . Volodymyr Nekrashevych . math/0510082 . Thurston equivalence of topological polynomials. Acta Mathematica . 2006 . 197 . 1–51 . 10.1007/s11511-006-0007-3.
  3. Web site: Period-n Rabbit Renormalization. 'Rabbit's show' by Evgeny Demidov . 2022-05-03 . 2022-05-03 . https://web.archive.org/web/20220503170632/https://www.ibiblio.org/e-notes/MSet/quadrat.htm . live.
  4. http://www.math.nagoya-u.ac.jp/~kawahira/works/rims0402.pdf Note on dynamically stable perturbations of parabolics by Tomoki Kawahira
  5. Web site: Twisted Three-Eared Rabbits: Identifying Topological Quadratics Up To Thurston Equivalence by Adam Chodof . 2022-05-03 . 2022-05-03 . https://web.archive.org/web/20220503093346/https://e.math.cornell.edu/people/belk/projects/AdamChodoff.pdf . live.
  6. Web site: Recent Research Papers (Only since 1999) Robert L. Devaney: Rabbits, Basilicas, and Other Julia Sets Wrapped in Sierpinski Carpets . 2020-04-07 . 2019-10-23 . https://web.archive.org/web/20191023110636/http://math.bu.edu/people/bob/papers.html . live.
  7. Web site: Polynomials, dynamics, and trees by Becca Winarski . 2022-05-08 . 2022-11-01 . https://web.archive.org/web/20221101023328/http://www.math.lsa.umich.edu/mathclub/winter2020/042320.pdf . live.
  8. Laurent Bartholdi . Volodymyr Nekrashevych . math/0510082v3 . Thurston equivalence of topological polynomials. 2005.
  9. 1906.07680v1 . Recognizing Topological Polynomials by Lifting Trees . James Belk . Justin Lanier . Dan Margalit . Rebecca R. Winarski. 2019 . math.DS.

External links