further exploring the parameter space of an ifs
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Further exploring the parameter space of an IFS Alden Walker - PowerPoint PPT Presentation

Further exploring the parameter space of an IFS Alden Walker (UChicago) Joint with Danny Calegari and Sarah Koch November 3, 2014 Recall: Sarah Koch spoke about this project on September 26. I will give essentially the same introduction, but


  1. Further exploring the parameter space of an IFS Alden Walker (UChicago) Joint with Danny Calegari and Sarah Koch November 3, 2014

  2. Recall: Sarah Koch spoke about this project on September 26. I will give essentially the same introduction, but I’ll discuss some different topics in the second half. Goal: Given dynamical systems parameterized by c ∈ C , connect features of the dynamics to features of the parameter space C and to other areas of math.

  3. Our dynamical systems of interest are iterated function systems : Iterated function systems (IFS): Let f 1 , · · · , f n : X → X , where X is a complete metric space, and all f i are contractions. Then { f 1 , . . . , f n } is an iterated function system . We are interested in the semi group generated by the f i . There is a unique invariant compact set Λ, the limit set of the IFS. (“Invariant” here means that Λ = � n i =1 f i Λ). (pictures from Wikipedia)

  4. Parameterized IFS For c ∈ C with | c | < 1, consider the IFS generated by the dilations ◮ f c ( z ) = cz − 1; (centered at α f = − 1 / (1 − c )) ◮ g c ( z ) = cz + 1; (centered at α g = 1 / (1 − c )) The limit set Λ c will have symmetry around ( α f + α g ) / 2 = 0 Note Λ c = f c Λ c ∪ g c Λ c ; we draw these sets in blue and orange.

  5. How to compute Λ c There are two simple ways to construct Λ c . Let G n be all words of length n in f c , g c . Method 1: Let p be any point in Λ c (for example the fixed point of f c , i.e. − 1 / (1 − c )). Then � Λ c = G n p n

  6. How to compute Λ c Method 2: Let D be a disk at 0 which is sent inside itself under f c and g c . Let � G n D = uD u ∈ G n Then for any n , we have Λ c ⊆ G n D , and � Λ c = G n D n ≥ 0

  7. Λ c D :

  8. Λ c D is sent inside itself under f c and g c :

  9. Λ c G 1 D , i.e. f c D ∪ g c D : Here 0 = f c , 1 = g c

  10. Λ c G 2 D , i.e. f c f c D ∪ f c g c D ∪ g c f c D ∪ g c g c D :

  11. Λ c G 3 D :

  12. Λ c G 4 D :

  13. Λ c G 8 D :

  14. Λ c G 12 D :

  15. Λ c Consider G n D (here G 3 D ). The limit set Λ c is a union of copies of Λ c , one in each disk in G n D :

  16. Parameterized IFS The parameter space for the IFS { f c , g c } is the open unit disk D . We define: M = { c ∈ D | Λ c is connected } M 0 = { c ∈ D | 0 ∈ Λ c } Lemma M 0 � M . Note the distinction with the Mandlebrot set; sets M and M 0 are different . Lemma (Bandt) c ∈ M ⇔ Λ c connected ⇔ Λ c is path connected ⇔ f c Λ c ∩ g c Λ c � = ∅

  17. M 0 � M c = 0 . 22 + 0 . 66 i is in M but not M 0 .

  18. Here is M :

  19. Here is M 0 :

  20. Sets M and M 0 together:

  21. Set M Set M has many interesting features:

  22. Holes Apparent holes in M are caused by f c Λ c and g c Λ c interlocking but not touching. (zoomed picture of Λ c )

  23. Sets M and M 0

  24. (fun with schottky )

  25. History Barnsley and Harrington (1985) defined sets M and M 0 and noted apparent holes in M Bousch 1988 Sets M and M 0 are connected and locally connected Odlyzko and Poonen 1993 Zeros of { 0 , 1 } polynomials (related to M 0 ) is connected and path connected Bandt 2002 Proved a hole in M , conjectured that the interior of M is dense away from the real axis Solomyak and Xu 2003 Proved that the interior is dense in a neighborhood of the imaginary axis Solomyak (several papers) proved interesting properties of M and M 0 , including a self-similarity result. Thurston 2013 Studied entropies of postcritically finite quadratic maps and produced a picture which, inside the unit disk, appears to be M 0 . Tiozzo 2013 Proved Thurston’s set is M 0 (inside the unit disk).

  26. Results Theorem There is an algorithm to certify that a point lies in the interior of M (and consequently to certify holes in M ; this is a very different method than Bandt’s certification of a hole) Theorem (Bandt’s Conjecture) The interior of M is dense in M away from the real axis. Theorem There is an infinite spiral of holes in M around the point ω ≈ 0 . 371859 + 0 . 519411 i. There are many infinite spirals of holes, and our method should work for any of them; we just happened to do it for ω .

  27. Properties of Λ c Recall: Lemma (Bousch) c ∈ M ( Λ c is connected) ⇔ f c Λ c ∩ g c Λ c � = ∅ . We prove: Lemma (The short hop lemma - CKW) If d ( f c Λ c , g c Λ c ) = δ , then for any two points p , q ∈ Λ c , there is a sequence of points p = s 0 , s 1 , . . . , s k = q such that s i ∈ Λ c and d ( s i , s i +1 ) ≤ δ .

  28. The short hop lemma If d ( f c Λ c , g c Λ c ) = δ , then for any two points p , q ∈ Λ c , there is a sequence of points p = s 0 , s 1 , . . . , s k = q such that s i ∈ Λ c and d ( s i , s i +1 ) ≤ δ .

  29. The short hop lemma If d ( f c Λ c , g c Λ c ) = δ , then for any two points p , q ∈ Λ c , there is a sequence of points p = s 0 , s 1 , . . . , s k = q such that s i ∈ Λ c and d ( s i , s i +1 ) ≤ δ .

  30. The short hop lemma If d ( f c Λ c , g c Λ c ) = δ , then for any two points p , q ∈ Λ c , there is a sequence of points p = s 0 , s 1 , . . . , s k = q such that s i ∈ Λ c and d ( s i , s i +1 ) ≤ δ .

  31. The short hop lemma If d ( f c Λ c , g c Λ c ) = δ , then for any two points p , q ∈ Λ c , there is a sequence of points p = s 0 , s 1 , . . . , s k = q such that s i ∈ Λ c and d ( s i , s i +1 ) ≤ δ .

  32. The short hop lemma If d ( f c Λ c , g c Λ c ) = δ , then for any two points p , q ∈ Λ c , there is a sequence of points p = s 0 , s 1 , . . . , s k = q such that s i ∈ Λ c and d ( s i , s i +1 ) ≤ δ .

  33. The short hop lemma If d ( f c Λ c , g c Λ c ) = δ , then for any two points p , q ∈ Λ c , there is a sequence of points p = s 0 , s 1 , . . . , s k = q such that s i ∈ Λ c and d ( s i , s i +1 ) ≤ δ .

  34. Traps Theorem There is an algorithm to certify that a point lies in the interior of M We’ll show there is an easy-to-check condition which certifies that f c Λ c ∩ g c Λ c � = ∅ , and thus that Λ c is connected, and this condition is open . This certificate is called a trap .

  35. Traps Suppose that f c Λ c and g c Λ c cross “transversely”:

  36. Traps ◮ Suppose that f c Λ c and g c Λ c cross transversely and that d ( f c Λ c , g c Λ c ) = δ . ◮ By lemma, there are short hop paths p 1 → p 2 in f c Λ c and q 1 → q 2 in g c Λ c , and these paths have gaps ≤ δ . ◮ The paths cross, so there is a pair of points, one in f c Λ and one in g c Λ c , with distance < δ . A contradiction unless δ = 0.

  37. Traps Note the existence of a trap is an open condition, so it certifies a parameter c as being in the interior of set M .

  38. Trap loops Since a trap is an open condition, each trap certifies a small ball as being in M . Using careful estimates, we can surround an apparent hole with these balls to rigorously certify it:

  39. Finding traps To find a trap, we want to show that f c Λ c is transverse to g c Λ c . It suffices to find two words u , v starting with f , g such that u Λ c is transverse to v Λ c :

  40. Finding traps It suffices to find two words u , v starting with f , g such that u Λ c is transverse to v Λ c . Here u = fffgffgfggfg , v = gggfgffgffgf The center of the disk D is 0, so the displacement vector between u Λ c and v Λ c is u (0) − v (0).

  41. Finding traps The displacement vector between u Λ c and v Λ c is u (0) − v (0). Note that rescaling the displacement: c − 12 ( u (0) − v (0)) Gives us the displacement vector relative to the original limit set Λ c :

  42. Finding traps If we consider Λ c , we can figure out what displacement vectors make it transverse: These are trap-like vectors for Λ c . We have shown: if u , v of length n start with f , g , and c − n ( u (0) − v (0)) is trap-like, then there is a trap for c .

  43. Finding traps We have shown: if u , v of length n start with f , g , and c − n ( u (0) − v (0)) is trap-like, then there is a trap for c . This is computationally useful, because trap-like vectors are trap-like for a whole ball of parameters. To find traps in a region in M , we can find trap-like vectors once ; then for a given parameter, find words u , v so c − n ( u (0) − v (0)) is trap-like.

  44. Finding traps We find trap-like vectors for this (quite small) region in parameter space. Then for every pixel, we search through pairs of words u , v trying to find a pair so c − n ( u (0) − v (0)) is trap-like. Left, the result of searching words through length 20. Right, through length 35.

  45. Similarity On the left is M near c = 0 . 371859 + 0 . 519411 i . On the right is a (zoomed) view of the set of differences between pairs of points in the limit set Λ c . This similarity is analogous to the Mandelbrot/Julia set similarity at Misiurewicz points: (picture by Tan Lei)

  46. Similarity On the left is M near the parameter 0 . 371859 + 0 . 519411 i . On the right is a (zoomed) view of the set of differences between pairs of points in the limit set Λ c . Theorem (Solomyak) These sets are asymptotically similar. (Small neighborhoods Hausdorff converge). We can re-prove this theorem (with a bonus: asymptotic interior!) using traps.

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