File:Siegel quadratic 3,2,1000,1... ,IIM.png

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Description
English: Julia set of quadratic polynomial with Siegel disc for rotation number [3,2,1000,1...]
Date
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Author Adam majewski
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This image shows main component of Julia set and its preimages under complex quadratic polynomial[1] up to level 100007. Main component :

  • contains Siegel disc ( around fixed point )
  • its boundary = critical orbit
  • it is a limit of iterations for every other component of filled Julia set

Algorithm[edit]

  • draw critical orbit = forward orbit of critical point ( "Iterates of critical point delineate a Siegel disc"[2])
  • for each point of critical orbit draw all its preimages up to LevelMax if Hit<HitLimit

Critical orbit in this case is : dense [3]( correct me if I'm wrong ) in boundary of component of filled-in Julia set containing Siegel disc.[4]


Mathemathical description[edit]

Description [5]

Quadratic polynomial [6] whose variable is a complex number

contains invariant Siegel disc  :

Boundary of Siegel disc

  • contains critical point  :
  • is a Jordan curve
  • is invariant under quadratic polynomial :
  • is a closure of forward orbits of critical points


Julia is build from preimages of boundary of Siegel disc ( union of copies of B meeting only at critical point and it's preimages ):[7]

Here maximal level is not infinity but finite number :

jMax = LevelMax = 100007;


rotation number[edit]

rotation number t is :[8]


In Maxima CAS one can compute it :

kill(all)$
a: [0,3,2,1000,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1]$
t:float(cfdisrep(a))$
l:%e^(2*%pi*%i*t)$
c:(l*(1-l/2))/2$
float(rectform(c))

So

t = .2857346725405882
c = 0.113891513213121  +0.595978335936124 i


How one can find limit of [3,2,1000,1,...] ?

Here is explanation of Bill Wood

"I don't know if Maxima knows much about the algebra of continued fractions, but it can be of some help hacking out the manipulation details of a derivation. A most useful fact is that

   [a1, a2, a3, ...] = a1 + 1/[a2, a3, ...]

provided the continued fraction converges. If we apply that three times by hand to [3, 2, 1000, 1, 1, ...] we obtain

   3 + 1/(2 + 1/(1000 + 1/[1, 1, ...]))

Now it is known that [1, 1, ...] converges to the Golden Ratio = (1+sqrt(5))/2. So now we can use Maxima as follows:

 (%i20) 3+(1/(2+(1/(1000+(1/((1+sqrt(5))/2))))));
                                    1
 (%o20)                    ---------------------- + 3
                                  1
                          ------------------ + 2
                               2
                          ----------- + 1000
                          sqrt(5) + 1
 (%i21) factor(%o13);
                              7003 sqrt(5) + 7017
 (%o21)                        -------------------
                              2001 sqrt(5) + 2005
 (%i22) %o21,numer;
 (%o22)                         3.499750279196346

You set a to [0, 3, 2, 1000, 1, 1, ...], which by our useful fact must be the reciprocal of [3, 2, 1000, 1, 1, ...], and indeed the reciprocal of 3.499750279196346 is 0.2857346725405882, which is what your float(t) evaluates to, so we seem to get consistent results.

If all of the continued fractions for the rotation numbers exhibited on the link you provided do end up repeating 1 forever then the method I used above can be used to determine their limits as ratios of linear expressions in sqrt(5)." Bill Wood

Centers of spirals[edit]

"In this example there are 7 big spirals around the Julia set. I guess this is because the rotation number is approximately [3, 2, 0, 0 , 0, ....] = 2/7.

I have checked that there is a 7-periodic point within each spiral, which will be slowly repelling. This shall be the center.

Other spirals will have preperiodic centers with period 7 and any preperiod. Maybe there are other smaller spirals at the Siegel disk belonging to higher periods, which correspond to truncating the continued fraction expansion later. " (Wolf Jung )

In program mandel[9]

  • press key b
  • input rotation number .2857346725405882
  • switch to dynamic plane ( F2 key)
  • increase iteration number ( key n ) up to 65 000
  • redraw
  • draw critical orbit ( key o) ( to draw full critical orbit, "you must recompile Mandel with a larger value of plotiter in calling drawOrbit() in qmnShell" )
  • find periodic point ( key x) for period 7
  • make forward iteraion of this point ( key f) to see that it is a periodic point








Angles of rays landing on period 7 orbit :

9/127
18/127
36/127
72/127
144-127=17/127
34/127
68/127

Compare with[edit]

C src code[edit]

References[edit]

  1. complex quadratic polynomial
  2. Complex Dynamics by Lennart Carleson and Theodore W. Gamelin. Page 84
  3. Dense set in wikipedia
  4. Joachim Grispolakis, John C. Mayer and Lex G. Oversteegen Journal: Trans. Amer. Math. Soc. 351 (1999), 1171-1201
  5. A. Blokh, X. Buff, A. Cheritat, L. Oversteegen The solar Julia sets of basic quadratic Cremer polynomials, Ergodic Theory and Dynamical Systems , 30 (2010), #1, 51-65,
  6. wikipedia : Complex quadratic polynomial
  7. Building blocks for Quadratic Julia sets by : Joachim Grispolakis, John C. Mayer and Lex G. Oversteegen Journal: Trans. Amer. Math. Soc. 351 (1999), 1171-1201
  8. Some examples of quadratic polynomial Siegel disks by Davoud Cheraghi
  9. Program mandel by Wolf Jung

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