slits spirals and loewner hulls
play

Slits, spirals and Loewner hulls Joan Lind University of Tennessee - PowerPoint PPT Presentation

Slits, spirals and Loewner hulls Joan Lind University of Tennessee The story begins Bieberbach conjecture (1916): For f ( z ) = z + a 2 z 2 + a 3 z 3 + conformal on D , then | a n | n . The story begins Bieberbach conjecture


  1. Slits, spirals and Loewner hulls Joan Lind University of Tennessee

  2. The story begins Bieberbach conjecture (1916): For f ( z ) = z + a 2 z 2 + a 3 z 3 + · · · conformal on D , then | a n | ≤ n .

  3. The story begins Bieberbach conjecture (1916): For f ( z ) = z + a 2 z 2 + a 3 z 3 + · · · conformal on D , then | a n | ≤ n . Charles Loewner introduced the Loewner equation in 1923 to prove the n = 3 case.

  4. The story begins Bieberbach conjecture (1916): For f ( z ) = z + a 2 z 2 + a 3 z 3 + · · · conformal on D , then | a n | ≤ n . Charles Loewner introduced the Loewner equation in 1923 to prove the n = 3 case. Louis des Branges again used the Loewner equation when he proved the conjecture in 1985.

  5. The story continues 0 Simple Random Walk (SRW) in 2 dimensions – has a conformally invariant scaling limit: 2-d Brownian motion

  6. The story continues Schramm’s question: Do other 2-dimensional random walks (such as SAW, LERW, etc.) have conformally invariant scaling limits? 0

  7. The story continues In 2000, Oded Schramm introduced SLE κ , a family of random processes that contain the possible conformally invariant scaling limits.

  8. The story continues In 2000, Oded Schramm introduced SLE κ , a family of random processes that contain the possible conformally invariant scaling limits. Through the Loewner equation, SLE κ correspond to √ κ B t .

  9. The Loewner equation L Equ ← ! growing families of 2-d sets real-valued functions

  10. From curves to functions γ ( t )

  11. From curves to functions γ ( t )

  12. From curves to functions g t γ ( t ) λ ( t )

  13. From curves to functions g t γ ( t ) λ ( t ) � 1 g t ( z ) = z + c t � z + O for z near infinity z 2

  14. From curves to functions g t γ ( t ) λ ( t ) � 1 g t ( z ) = z + 2 t � z + O for z near infinity z 2

  15. From curves to functions g t γ ( t ) λ ( t ) ∂ 2 ∂ t g t ( z ) = g t ( z ) − λ ( t )

  16. From functions to growing families of sets For a continuous, real-valued function λ ( t ) and z ∈ H , consider ∂ 2 ∂ t g t ( z ) = g t ( z ) − λ ( t ) , g 0 ( z ) = z

  17. From functions to growing families of sets For a continuous, real-valued function λ ( t ) and z ∈ H , consider ∂ 2 ∂ t g t ( z ) = g t ( z ) − λ ( t ) , g 0 ( z ) = z Loewner hulls: K t = { z ∈ H : g s ( z ) = λ ( s ) for some s ≤ t } .

  18. From functions to growing families of sets For a continuous, real-valued function λ ( t ) and z ∈ H , consider ∂ 2 ∂ t g t ( z ) = g t ( z ) − λ ( t ) , g 0 ( z ) = z Loewner hulls: K t = { z ∈ H : g s ( z ) = λ ( s ) for some s ≤ t } . Theorem: g t is a conformal map from H \ K t onto H .

  19. Loewner flow ∂ t g t ( z ) = 2 Re g t ( z ) − λ ( t ) ∂ Im g t ( z ) | g t ( z ) − λ ( t ) | 2 − 2 i | g t ( z ) − λ ( t ) | 2 1 0.8 0.6 0.4 0.2 –1 –0.5 0.5 1

  20. Example Loewner hull generated by λ ( t ) ≡ 0.

  21. Loewner equation L Equ ← ! growing families of 2-d sets real-valued functions

  22. The geometry of SLE curves L Equ √ κ B t SLE κ ← →

  23. The geometry of SLE curves L Equ √ κ B t SLE κ ← → 0 ≤ κ ≤ 4 4 < κ < 8 8 ≤ κ

  24. The geometry of SLE curves SLE 2 SLE 6

  25. Simple curve Loewner hulls Question: When does the deterministic Loewner equation generate a simple curve?

  26. Simple curve Loewner hulls Question: When does the deterministic Loewner equation generate a simple curve? Lip(1 / 2) functions: | λ ( t ) − λ ( s ) | ≤ M | t − s | 1 / 2 for all t , s is the domain of λ. The smallest such M is || λ || 1 / 2 .

  27. Simple curve Loewner hulls Question: When does the deterministic Loewner equation generate a simple curve? Lip(1 / 2) functions: | λ ( t ) − λ ( s ) | ≤ M | t − s | 1 / 2 for all t , s is the domain of λ. The smallest such M is || λ || 1 / 2 . Answer: (Marshall, Rohde) There exists C 0 > 0 so that for λ ∈ Lip(1 / 2) with || λ || 1 / 2 < C 0 , then the Loewner hull is a quasislit γ .

  28. Simple curve Loewner hulls Question: Do all Lip(1 / 2) driving functions generate simple curves?

  29. Simple curve Loewner hulls Question: Do all Lip(1 / 2) driving functions generate simple curves? Answer: (Marshall, Rohde) No. There is a non-simple example (a curve that spirals around a disc) that is generated by a Lip(1 / 2) driving function.

  30. Simple curve Loewner hulls Question: What is the optimal value of C 0 for the Marshall-Rohde theorem?

  31. Simple curve Loewner hulls Question: What is the optimal value of C 0 for the Marshall-Rohde theorem? Answer: (L) C 0 = 4.

  32. Simple curve Loewner hulls Question: What is the optimal value of C 0 for the Marshall-Rohde theorem? Answer: (L) C 0 = 4. Key examples: λ ( t ) = − c √ 1 − t c = 3 c = 5

  33. Loewner deformations Omer Angel’s question: For r < 1, what can you say about Loewner hull driven by r λ ?

  34. Loewner deformations Omer Angel’s question: For r < 1, what can you say about Loewner hull driven by r λ ? Is it at least as nice as the hull driven by λ ?

  35. Loewner deformations Omer Angel’s question: For r < 1, what can you say about Loewner hull driven by r λ ? Is it at least as nice as the hull driven by λ ? This is true for SLE. 0 ≤ κ ≤ 4 4 < κ < 8 8 ≤ κ

  36. Loewner deformations Omer Angel’s question: For r < 1, what can you say about Loewner hull driven by r λ ? Is it at least as nice as the hull driven by λ ? This is true for λ ( t ) = − c √ 1 − t . c = 3 c = 5

  37. Loewner deformations Omer Angel’s question: For r < 1, what can you say about Loewner hull driven by r λ ? Is it at least as nice as the hull driven by λ ? Is it always true?

  38. Loewner deformations Omer Angel’s question: For r < 1, what can you say about Loewner hull driven by r λ ? Is it at least as nice as the hull driven by λ ? Is it always true? Answer: N0.

  39. Loewner deformations Theorem (L, Marshall, Rohde) Let λ be the driving function for the star spiral. When 0 < r < 1 , then r λ generates a simple curve, and when r > 1 , then r λ generates a “bubble” curve.

  40. Spirals and collisions Theorem (L, Marshall, Rohde) If γ is a suffiently nice infinite spiral of half-plane capacity T, or if γ has a tangential self-intersection, then its driving term λ satisfies | λ ( T ) − λ ( t ) | lim √ = 4 . T − t t → T

  41. Spirals and collisions Theorem (L, Marshall, Rohde) If γ is a suffiently nice infinite spiral of half-plane capacity T, or if γ has a tangential self-intersection, then its driving term λ satisfies | λ ( T ) − λ ( t ) | lim √ = 4 . T − t t → T Theorem (L, Marshall, Rohde) If λ : [0 , T ] → R is sufficiently regular on [0 , T ) and if | λ ( T ) − λ ( t ) | √ lim = κ > 4 , T − t t → T then γ ( T ) = lim t → T γ ( t ) exists, is real, and γ intersects R in the same angle as the trace for κ √ 1 − t.

  42. Spirals and collisions Scaling Property: ◮ If λ generates hull K t , then c λ ( t / c 2 ) generates cK t / c 2 .

  43. Spirals and collisions Scaling Property: ◮ If λ generates hull K t , then c λ ( t / c 2 ) generates cK t / c 2 . Example: λ ( t ) = c √ t

  44. Spirals and collisions Concatenation Property: ◮ If λ generates hull K t for t ∈ [0 , T ], then λ restricted to [ t 0 , T ] generates hull g t 0 ( K T \ K t 0 ).

  45. Spirals and collisions Concatenation Property: ◮ If λ generates hull K t for t ∈ [0 , T ], then λ restricted to [ t 0 , T ] generates hull g t 0 ( K T \ K t 0 ). g t 0 g t 0 ( K T \ K t 0 ) K t 0 λ (0) λ ( t 0 )

  46. Spirals and collisions Start with λ = − c √ 1 − t . For t 0 ∈ (0 , 1), map down by g t 0 . Rescale by 1 / √ 1 − t 0 .

  47. Spirals and collisions Start with λ = − c √ 1 − t . For t 0 ∈ (0 , 1), map down by g t 0 . Rescale by 1 / √ 1 − t 0 . What do we obtain? The same hull that we started with.

  48. Spirals and collisions Start with λ satisfying | λ (1) − λ ( t ) | lim √ 1 − t = κ ≥ 4 t → 1 Shift so that λ (1) = 0. For t 0 ∈ (0 , 1), map down by g t 0 . Rescale by 1 / √ 1 − t 0 .

  49. Spirals and collisions Start with λ satisfying | λ (1) − λ ( t ) | lim √ 1 − t = κ ≥ 4 t → 1 Shift so that λ (1) = 0. For t 0 ∈ (0 , 1), map down by g t 0 . Rescale by 1 / √ 1 − t 0 . What do we obtain? A hull that is getting closer and closer to the hull generated by ± κ √ 1 − t .

  50. Spirals and collisions What happens when κ = 4?

  51. Spirals and collisions What happens when κ = 4? 4 √ 1 − t generates a hull that intersects the real line tangentially.

  52. Spirals and collisions What happens when κ = 4? 4 √ 1 − t generates a hull that intersects the real line tangentially. The spiral behavior can be viewed as tangential behavior.

  53. Recap: the Loewner equation question L Equ ← ! growing families of 2-d sets real-valued functions Question: How do properties of the functions relate to geometric characteristics of the sets?

  54. Sample of other Loewner explorations

  55. Sample of other Loewner explorations ◮ Spacefilling curves (L, Rohde)

  56. Sample of other Loewner explorations ◮ Spacefilling curves (L, Rohde) ◮ Driving functions with higher regularity (Wong, L, Tran)

Download Presentation
Download Policy: The content available on the website is offered to you 'AS IS' for your personal information and use only. It cannot be commercialized, licensed, or distributed on other websites without prior consent from the author. To download a presentation, simply click this link. If you encounter any difficulties during the download process, it's possible that the publisher has removed the file from their server.

Recommend


More recommend