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Asymptotic counting in dynamical systems Alan Yan 1 Mentor: Sergiy Merenkov 2 1 West-Windsor Plainsboro High School North 2 CCNY-CUNY April 19-20, 2018 MIT PRIMES Conference Asymptotic counting in dynamical systems 1 / 22

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Page 1: Asymptotic counting in dynamical systemsmath.mit.edu/research/highschool/primes/materials/2018... · 2018-05-23 · Asymptotic counting in dynamical systems Alan Yan 1 Mentor: Sergiy

Asymptotic counting in dynamical systems

Alan Yan 1

Mentor: Sergiy Merenkov 2

1West-Windsor Plainsboro High School North

2CCNY-CUNY

April 19-20, 2018MIT PRIMES Conference

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Introduction

Question

Given a counting function which quantifies some measurable property of ageometric object, what are the asymptotics of such a function?

Expectation: ∼ cxd , d is “dimension”

Two Main Examples

Fatou Components of Rational MapsLimit Sets of Schottky Groups

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Dimension

Definition (Box-Counting Dimension)

Suppose that N(ε) is the number of boxes of side length ε required tocover a set S . Then the dimension of S is defined as

limε→0

logN(ε)

log(1/ε).

unique d such that N(1/x) ∼ cxd as x →∞.

motivation for power law

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Dimension Example: East Coast of Britain

Figure: East Coast of Britain, d ≈ 1.21

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Dimension Example: Cantor Set

Figure: Cantor Set, d = log3 2

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Julia Set and Fatou Components

Definition

The filled-in Julia set of a complex function f is defined as

K (f ) = {z ∈ C : f k(z) 9∞}.

Definition

The Julia Set of f is defined as the boundary of the filled-in Julia set, i.e.

J(F ) = ∂K (F ).

Definition

A Fatou component of f is a connected component of K (f ).

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Examples: Julia set of f (z) = z2 + c

Figure: c = −0.74543 + 0.11301i

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Examples: Julia set of f (z) = z2 + c

Figure: The Basilica (c = −1)

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Main Theorem on Fatou Components

Definition

Given a set X ⊂ C, define the diameter of X as

diam(X ) = sup{|x − y | : x , y ∈ X}.

The Counting Function

For every function f : C→ C, we associate a counting functionNf : R>0 → R≥0 where Nf (x) is the number of Fatou components of fwhose diameter is at least 1/x .

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Main Result on Fatou Components Cont.

Conjecture

Suppose f (z) = z2 + c has an infinite number of Fatou components. Then,

Nf (x) ∼ cf xd

where d is the dimension of J(f ) and cf > 0 is a constant.

Numerically verified the theorem for f (z) = z2 − 1.

Proved in paper by M. Pollicott, M. Urbanski

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Algorithm: Diameters of the Basilica

Escaping Criterion

Let f (z) = z2 + c be a complex quadratic function. Let R =1+√

1+4|c|2 . If

for some n > 0 we have |f n(z0)| > R, then z0 6∈ K (f ).

1 Construction

2 Distinguish Components

3 Computation of Diameter

4 Problem with (2): Bridges

5

√A Counting Function

Figure: Bridge

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Hyperbolic Geometry: The Poincare Disk Model

Definition

The Poincare disk is the unit disk D equipped with new notions of lines,distance, and angles.

Geodesics are orthogonal circles!

To calculate distance, we canuse the formula

d(A,B) = ln|AQ| · |BP||AP| · |BQ|

Figure: Geodesics

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Angles in D

Figure: Angle between Geodesics

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Isometries and Schottky Groups

Definition

An isometry is a map that preserves distances.

Isometry Groups

G =

{h(z) =

αz + β

βz + α: |α|2 − |β|2 = 1, α, β ∈ D

}.

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Isometries and Schottky Groups (Contd)

Definition

If g is an isometry which does fix z0, then Dz0(g) = D(g) represents theclosed half-plane in D bounded by the perpendicular bisector of thehyperbolic segment [z0, g(z0)] containing g(z0).

Definition

A Schottky group of rank 2 is a subgroup of G generated by twoisometries g1, g2 that satisfies

(D(g1) ∪ D(g−11 )) ∩ (D(g2) ∪ D(g−12 ) = ∅

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Example: Schottky Groups

Figure: Induced Half Planes of the Generators

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The Limit Set of a Schottky Group

Definition

The limit set of L(Γ) of a isometry group Γ is defined by

L(Γ) = Γz ∩ ∂D

Figure: L(S(g1, g2))

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Conjecture on the Limit Sets S(g1, g2)

Definition (Counting Function)

For a Schottky group S(g1, g2), define N(x , p) : R>0 × D→ R≥0 to bethe number of intervals I ∈ ∂D\L(S(g1, g2)) such that the angle betweenthe geodesics from the endpoints of I to p is at least 1/x .

Conjecture

For every point p ∈ D and nontrivial Schottky group S(g1, g2),

N(x , p) ∼ cxd

where d is the dimension of L(S(g1, g2)). The constant c depends on thepoint p.

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Future Research

Fatou Components

Generalize the theorem for different types of rational mapsProve a similar theorem replacing diameters by

√A.

Limits Sets of Schottky Groups

Efficient Algorithm for limit sets of Schottky groupsverify and prove the conjecture on Schottky groupsRelationship between c and p

Discover new counting functions which are asymptotic to cxd .

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Acknowledgements

MIT-PRIMES Program

Prof. Sergiy Merenkov

Dr. Tanya Khovanova

My parents

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References

1 Dal’bo-Milonet, F. (2011). Geodesic and horocyclic trajectories.London: Springer.

2 M. Pollicott, M. Urbanski, Asymptotic Counting in ConformalDynamical Systems (2017)

3 A. Kontorovich, H. Oh, Apollonian Circle Packings and ClosedHorospheres on Hyperbolic 3-Manifolds

4 Carleson, L., Gamelin, T. (1993). Complex dynamics. New York:Springer-Verlag.

5 Falconer, K. (2003). Fractal geometry : mathematical foundationsand applications. Chichester: Wiley.

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Image Sources

1 Alexis Monnerot-Dumaine / CC-BY-SA-3.0 (1)

2 Adam Majewski / CC-BY-SA-3.0 (3)

3 Dal’bo-Milonet, F. (2011). Geodesic and horocyclic trajectories.London: Springer. (8, 9)

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