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Complex dynamics: the intriguing case of wandering domains Gwyneth - - PowerPoint PPT Presentation
Complex dynamics: the intriguing case of wandering domains Gwyneth - - PowerPoint PPT Presentation
Complex dynamics: the intriguing case of wandering domains Gwyneth Stallard The Open University Joint work with Anna Miriam Benini, Vasiliki Evdoridou, Nuria Fagella and Phil Rippon Barcelona March 2019 Basic definitions f : C C is
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Basic definitions
f : C → C is analytic Definition The Fatou set (or stable set) is F(f) = {z : (f n) is equicontinuous in some neighbourhood of z}.
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Basic definitions
f : C → C is analytic Definition The Fatou set (or stable set) is F(f) = {z : (f n) is equicontinuous in some neighbourhood of z}. The Fatou set is open and z ∈ F(f) ⇐ ⇒ f(z) ∈ F(f).
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Basic definitions
f : C → C is analytic Definition The Fatou set (or stable set) is F(f) = {z : (f n) is equicontinuous in some neighbourhood of z}. The Fatou set is open and z ∈ F(f) ⇐ ⇒ f(z) ∈ F(f). Definition The Julia set (or chaotic set) is J(f) = C \ F(f).
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Components of the Fatou set
Let U be a component of the Fatou set (a Fatou component),
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Components of the Fatou set
Let U be a component of the Fatou set (a Fatou component), and let Un denote the Fatou component containing f n(U).
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Components of the Fatou set
Let U be a component of the Fatou set (a Fatou component), and let Un denote the Fatou component containing f n(U). U is periodic with period p if Up = U and Un = U for 1 ≤ n < p.
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Components of the Fatou set
Let U be a component of the Fatou set (a Fatou component), and let Un denote the Fatou component containing f n(U). U is periodic with period p if Up = U and Un = U for 1 ≤ n < p. U is pre-periodic if Um is periodic for some m ∈ N.
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Components of the Fatou set
Let U be a component of the Fatou set (a Fatou component), and let Un denote the Fatou component containing f n(U). U is periodic with period p if Up = U and Un = U for 1 ≤ n < p. U is pre-periodic if Um is periodic for some m ∈ N. U is a wandering domain if Um = Un for all m = n.
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Components of the Fatou set
Let U be a component of the Fatou set (a Fatou component), and let Un denote the Fatou component containing f n(U). U is periodic with period p if Up = U and Un = U for 1 ≤ n < p. U is pre-periodic if Um is periodic for some m ∈ N. U is a wandering domain if Um = Un for all m = n. Periodic Fatou components are well understood and there is a classification essentially due to Fatou and Cremer (1920s).
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Classification of invariant Fatou components
Attracting basin
Type 1: U is an attracting basin
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Classification of invariant Fatou components
Attracting basin
Type 1: U is an attracting basin g(z) = z2 − 1 f = g2 has an attracting basin
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Classification of invariant Fatou components
Attracting basin
Type 1: U is an attracting basin g(z) = z2 − 1 f = g2 has an attracting basin U contains an attracting fixed point z0: f(z0) = z0, |f ′(z0)| < 1
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Classification of invariant Fatou components
Attracting basin
Type 1: U is an attracting basin g(z) = z2 − 1 f = g2 has an attracting basin U contains an attracting fixed point z0: f(z0) = z0, |f ′(z0)| < 1 f n(z) → z0 for z ∈ U
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Classification of invariant Fatou components
Attracting basin
Type 1: U is an attracting basin g(z) = z2 − 1 f = g2 has an attracting basin U contains an attracting fixed point z0: f(z0) = z0, |f ′(z0)| < 1 f n(z) → z0 for z ∈ U U is super-attracting if f ′(z0) = 0
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Classification of invariant Fatou components
Parabolic basin
Type 2: U is a parabolic basin
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Classification of invariant Fatou components
Parabolic basin
Type 2: U is a parabolic basin f(z) = z2 + 0.25
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Classification of invariant Fatou components
Parabolic basin
Type 2: U is a parabolic basin f(z) = z2 + 0.25 ∂U contains a parabolic fixed point z0: f(z0) = z0, f ′(z0) = 1
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Classification of invariant Fatou components
Parabolic basin
Type 2: U is a parabolic basin f(z) = z2 + 0.25 ∂U contains a parabolic fixed point z0: f(z0) = z0, f ′(z0) = 1 f n(z) → z0 for z ∈ U
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Classification of invariant Fatou components
Siegel disc
Type 3: U is a Siegel disc
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Classification of invariant Fatou components
Siegel disc
Type 3: U is a Siegel disc f(z) = e2πi(1−
√ 5)/2z(z − 1)
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Classification of invariant Fatou components
Siegel disc
Type 3: U is a Siegel disc f(z) = e2πi(1−
√ 5)/2z(z − 1)
U contains a fixed point z0: f(z0) = z0, f ′(z0) = e2πiθ, θ is irrational
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Classification of invariant Fatou components
Siegel disc
Type 3: U is a Siegel disc f(z) = e2πi(1−
√ 5)/2z(z − 1)
U contains a fixed point z0: f(z0) = z0, f ′(z0) = e2πiθ, θ is irrational f : U → U is conjugate to an irrational rotation of the disc
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Classification of invariant Fatou components
Baker domain
Type 4: U is a Baker domain
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Classification of invariant Fatou components
Baker domain
Type 4: U is a Baker domain f(z) = z + 1 + e−z
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Classification of invariant Fatou components
Baker domain
Type 4: U is a Baker domain f(z) = z + 1 + e−z For z ∈ U, f n(z) tends to an essential singularity
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Classification of invariant Fatou components
Baker domain
Type 4: U is a Baker domain f(z) = z + 1 + e−z For z ∈ U, f n(z) tends to an essential singularity This type cannot occur for polynomials
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The existence of wandering domains
Theorem (Sullivan, 1982) If f is rational, then f has no wandering domains.
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The existence of wandering domains
Theorem (Sullivan, 1982) If f is rational, then f has no wandering domains. Corollary There is a complete classification of the behaviour in Fatou components of rational functions
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The existence of wandering domains
Theorem (Sullivan, 1982) If f is rational, then f has no wandering domains. Corollary There is a complete classification of the behaviour in Fatou components of rational functions Wandering domains do exist for transcendental entire functions, and are not well understood.
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Early examples of wandering domains
Herman (1984) gave simple examples of functions with simply connected wandering domains
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Early examples of wandering domains
Herman (1984) gave simple examples of functions with simply connected wandering domains e.g. f(z) = z − 1 + e−z + 2πi has a wandering attracting basin.
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Early examples of wandering domains
Herman (1984) gave simple examples of functions with simply connected wandering domains e.g. f(z) = z − 1 + e−z + 2πi has a wandering attracting basin.
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Early examples of wandering domains
Herman (1984) gave simple examples of functions with simply connected wandering domains e.g. f(z) = z − 1 + e−z + 2πi has a wandering attracting basin. Baker gave the first example of a wandering domain.
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Early examples of wandering domains
Herman (1984) gave simple examples of functions with simply connected wandering domains e.g. f(z) = z − 1 + e−z + 2πi has a wandering attracting basin. Baker gave the first example of a wandering domain.
- In 1963 he constructed an infinite product f and a nested
sequence of annuli An tending to infinity with f(An) ⊂ An+1.
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Early examples of wandering domains
Herman (1984) gave simple examples of functions with simply connected wandering domains e.g. f(z) = z − 1 + e−z + 2πi has a wandering attracting basin. Baker gave the first example of a wandering domain.
- In 1963 he constructed an infinite product f and a nested
sequence of annuli An tending to infinity with f(An) ⊂ An+1.
- In 1976 he showed that these annuli belong to distinct
Fatou components (multiply connected wandering domains).
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Multiply connected wandering domains
Theorem (Baker, 1984) If U is a multiply connected Fatou component then U is a wandering domain
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Multiply connected wandering domains
Theorem (Baker, 1984) If U is a multiply connected Fatou component then U is a wandering domain Un+1 surrounds Un, for large n Un → ∞ as n → ∞.
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Multiply connected wandering domains
Theorem (Baker, 1984) If U is a multiply connected Fatou component then U is a wandering domain Un+1 surrounds Un, for large n Un → ∞ as n → ∞. Theorem (Zheng, 2006) If U is a multiply connected wandering domain then there exist sequences (rn) and (Rn) such that, for large n, Un ⊃ {z : rn ≤ |z| ≤ Rn}
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Multiply connected wandering domains
Theorem (Baker, 1984) If U is a multiply connected Fatou component then U is a wandering domain Un+1 surrounds Un, for large n Un → ∞ as n → ∞. Theorem (Zheng, 2006) If U is a multiply connected wandering domain then there exist sequences (rn) and (Rn) such that, for large n, Un ⊃ {z : rn ≤ |z| ≤ Rn} and Rn/rn → ∞ as n → ∞.
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Dynamical behaviour in multiply connected wandering domains
Theorem (Bergweiler, Rippon and Stallard, 2013) If U is a multiply connected wandering domain then for large n ∈ N, there is an absorbing annulus Bn = A(r an
n , r bn n ) ⊂ Un
with lim infn→∞ bn/an > 1
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Dynamical behaviour in multiply connected wandering domains
Theorem (Bergweiler, Rippon and Stallard, 2013) If U is a multiply connected wandering domain then for large n ∈ N, there is an absorbing annulus Bn = A(r an
n , r bn n ) ⊂ Un
with lim infn→∞ bn/an > 1 such that, for every compact set C ⊂ U, f n(C) ⊂ Bn for n ≥ N(C).
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Dynamical behaviour in multiply connected wandering domains
Theorem (Bergweiler, Rippon and Stallard, 2013) If U is a multiply connected wandering domain then for large n ∈ N, there is an absorbing annulus Bn = A(r an
n , r bn n ) ⊂ Un
with lim infn→∞ bn/an > 1 such that, for every compact set C ⊂ U, f n(C) ⊂ Bn for n ≥ N(C). f behaves like a large degree monomial inside Bn.
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Dynamical behaviour in multiply connected wandering domains
Theorem (Bergweiler, Rippon and Stallard, 2013) If U is a multiply connected wandering domain then for large n ∈ N, there is an absorbing annulus Bn = A(r an
n , r bn n ) ⊂ Un
with lim infn→∞ bn/an > 1 such that, for every compact set C ⊂ U, f n(C) ⊂ Bn for n ≥ N(C). f behaves like a large degree monomial inside Bn. This led to progress on a longstanding question as to whether f ◦ g = g ◦ f implies J(f) = J(g) (Benini, Rippon and Stallard).
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Classifying simply connected wandering domains
EPSRC funded project
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Classifying simply connected wandering domains
EPSRC funded project
Gwyneth Stallard Phil Rippon Vasso Evdoridou Nuria Fagella Anna Benini
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Background - orbits of simply connected wandering domains
There are three possible types of orbits of a wandering domain U containing a point z.
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Background - orbits of simply connected wandering domains
There are three possible types of orbits of a wandering domain U containing a point z. Escaping (f n(z) → ∞)
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Background - orbits of simply connected wandering domains
There are three possible types of orbits of a wandering domain U containing a point z. Escaping (f n(z) → ∞)
- most known examples are of this type and are escaping
versions of periodic components.
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Background - orbits of simply connected wandering domains
There are three possible types of orbits of a wandering domain U containing a point z. Escaping (f n(z) → ∞)
- most known examples are of this type and are escaping
versions of periodic components.
Oscillating ((f n(z)) has bounded and unbounded subsequences)
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Background - orbits of simply connected wandering domains
There are three possible types of orbits of a wandering domain U containing a point z. Escaping (f n(z) → ∞)
- most known examples are of this type and are escaping
versions of periodic components.
Oscillating ((f n(z)) has bounded and unbounded subsequences)
- Eremenko and Lyubich (1987) constructed examples using
approximation theory
- Bishop (2015) constructed examples using quasiconformal
folding
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Background - orbits of simply connected wandering domains
There are three possible types of orbits of a wandering domain U containing a point z. Escaping (f n(z) → ∞)
- most known examples are of this type and are escaping
versions of periodic components.
Oscillating ((f n(z)) has bounded and unbounded subsequences)
- Eremenko and Lyubich (1987) constructed examples using
approximation theory
- Bishop (2015) constructed examples using quasiconformal
folding
Bounded ((f n(z)) is bounded)
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Background - orbits of simply connected wandering domains
There are three possible types of orbits of a wandering domain U containing a point z. Escaping (f n(z) → ∞)
- most known examples are of this type and are escaping
versions of periodic components.
Oscillating ((f n(z)) has bounded and unbounded subsequences)
- Eremenko and Lyubich (1987) constructed examples using
approximation theory
- Bishop (2015) constructed examples using quasiconformal
folding
Bounded ((f n(z)) is bounded)
- Not known if these can exist
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Escaping wandering domains
Question Are all escaping wandering domains escaping versions of periodic Fatou components?
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Escaping wandering domains
Question Are all escaping wandering domains escaping versions of periodic Fatou components? Wandering attracting domain f(z) = z + sin z + 2π
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Escaping wandering domains
Question Are all escaping wandering domains escaping versions of periodic Fatou components? Wandering attracting domain f(z) = z + sin z + 2π Wandering parabolic domain f(z) = z cos z + 2π
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Escaping wandering domains
Question Are all escaping wandering domains escaping versions of periodic Fatou components? Wandering attracting domain f(z) = z + sin z + 2π Wandering parabolic domain f(z) = z cos z + 2π Answer No - everything seems possible!
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Classifying simply connected wandering domains
Hyperbolic contraction
Theorem Let U be a simply connected wandering domain and suppose z, w ∈ U have distinct orbits. Then there are three possibilities.
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Classifying simply connected wandering domains
Hyperbolic contraction
Theorem Let U be a simply connected wandering domain and suppose z, w ∈ U have distinct orbits. Then there are three possibilities.
1 U is contracting: for all such pairs z, w ∈ U,
ρUn(f n(z), f n(w)) decreases to 0.
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Classifying simply connected wandering domains
Hyperbolic contraction
Theorem Let U be a simply connected wandering domain and suppose z, w ∈ U have distinct orbits. Then there are three possibilities.
1 U is contracting: for all such pairs z, w ∈ U,
ρUn(f n(z), f n(w)) decreases to 0.
2 U is semi-contracting: for all such pairs z, w ∈ U,
ρUn(f n(z), f n(w)) decreases to c(z, w) > 0.
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Classifying simply connected wandering domains
Hyperbolic contraction
Theorem Let U be a simply connected wandering domain and suppose z, w ∈ U have distinct orbits. Then there are three possibilities.
1 U is contracting: for all such pairs z, w ∈ U,
ρUn(f n(z), f n(w)) decreases to 0.
2 U is semi-contracting: for all such pairs z, w ∈ U,
ρUn(f n(z), f n(w)) decreases to c(z, w) > 0.
3 U is eventually isometric: for all such pairs z, w ∈ U,
ρUn(f n(z), f n(w)) is eventually constant.
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Classifying simply connected wandering domains
Hyperbolic contraction
Theorem Let U be a simply connected wandering domain and suppose z, w ∈ U have distinct orbits. Then there are three possibilities.
1 U is contracting: for all such pairs z, w ∈ U,
ρUn(f n(z), f n(w)) decreases to 0.
2 U is semi-contracting: for all such pairs z, w ∈ U,
ρUn(f n(z), f n(w)) decreases to c(z, w) > 0.
3 U is eventually isometric: for all such pairs z, w ∈ U,
ρUn(f n(z), f n(w)) is eventually constant. A wandering domain that is the lift of an attracting basin / parabolic basin / Siegel disc is
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Classifying simply connected wandering domains
Hyperbolic contraction
Theorem Let U be a simply connected wandering domain and suppose z, w ∈ U have distinct orbits. Then there are three possibilities.
1 U is contracting: for all such pairs z, w ∈ U,
ρUn(f n(z), f n(w)) decreases to 0.
2 U is semi-contracting: for all such pairs z, w ∈ U,
ρUn(f n(z), f n(w)) decreases to c(z, w) > 0.
3 U is eventually isometric: for all such pairs z, w ∈ U,
ρUn(f n(z), f n(w)) is eventually constant. A wandering domain that is the lift of an attracting basin / parabolic basin / Siegel disc is contracting
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Classifying simply connected wandering domains
Hyperbolic contraction
Theorem Let U be a simply connected wandering domain and suppose z, w ∈ U have distinct orbits. Then there are three possibilities.
1 U is contracting: for all such pairs z, w ∈ U,
ρUn(f n(z), f n(w)) decreases to 0.
2 U is semi-contracting: for all such pairs z, w ∈ U,
ρUn(f n(z), f n(w)) decreases to c(z, w) > 0.
3 U is eventually isometric: for all such pairs z, w ∈ U,
ρUn(f n(z), f n(w)) is eventually constant. A wandering domain that is the lift of an attracting basin / parabolic basin / Siegel disc is contracting / contracting
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Classifying simply connected wandering domains
Hyperbolic contraction
Theorem Let U be a simply connected wandering domain and suppose z, w ∈ U have distinct orbits. Then there are three possibilities.
1 U is contracting: for all such pairs z, w ∈ U,
ρUn(f n(z), f n(w)) decreases to 0.
2 U is semi-contracting: for all such pairs z, w ∈ U,
ρUn(f n(z), f n(w)) decreases to c(z, w) > 0.
3 U is eventually isometric: for all such pairs z, w ∈ U,
ρUn(f n(z), f n(w)) is eventually constant. A wandering domain that is the lift of an attracting basin / parabolic basin / Siegel disc is contracting / contracting / isometric.
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Proof of hyperbolic contraction classification
Pick a base point z0 ∈ U.
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Proof of hyperbolic contraction classification
Pick a base point z0 ∈ U. Let φn : Un → D denote a Riemann mapping with φ(f n(z0)) = 0.
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Proof of hyperbolic contraction classification
Pick a base point z0 ∈ U. Let φn : Un → D denote a Riemann mapping with φ(f n(z0)) = 0. Consider the sequence of inner functions gn = φnfφ−1
n−1.
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Proof of hyperbolic contraction classification
Pick a base point z0 ∈ U. Let φn : Un → D denote a Riemann mapping with φ(f n(z0)) = 0. Consider the sequence of inner functions gn = φnfφ−1
n−1.
Show that the rate of contraction depends on the values of g′
n(0) - using techniques of Beardon and Carne.
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Proof of hyperbolic contraction classification
Pick a base point z0 ∈ U. Let φn : Un → D denote a Riemann mapping with φ(f n(z0)) = 0. Consider the sequence of inner functions gn = φnfφ−1
n−1.
Show that the rate of contraction depends on the values of g′
n(0) - using techniques of Beardon and Carne. ∞
- n=0
(1 − |g′
n(0)|) = ∞ ⇐
⇒ gn(w) → 0 as n → ∞ for all w ∈ D.
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Contracting wandering domains
Recall U is contracting if ∞
n=0(1 − |g′ n(0)|) = ∞.
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Contracting wandering domains
Recall U is contracting if ∞
n=0(1 − |g′ n(0)|) = ∞.
This implies that, for w ∈ D, gn(w) → 0 as n → ∞.
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Contracting wandering domains
Recall U is contracting if ∞
n=0(1 − |g′ n(0)|) = ∞.
This implies that, for w ∈ D, gn(w) → 0 as n → ∞. U is strongly contracting if lim sup 1
n
n
k=1 |g′ k(0)| = d < 1
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Contracting wandering domains
Recall U is contracting if ∞
n=0(1 − |g′ n(0)|) = ∞.
This implies that, for w ∈ D, gn(w) → 0 as n → ∞. U is strongly contracting if lim sup 1
n
n
k=1 |g′ k(0)| = d < 1
- This implies that, for w ∈ D, |gn(w)| ≤ (d + ǫ)n, for large n.
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Contracting wandering domains
Recall U is contracting if ∞
n=0(1 − |g′ n(0)|) = ∞.
This implies that, for w ∈ D, gn(w) → 0 as n → ∞. U is strongly contracting if lim sup 1
n
n
k=1 |g′ k(0)| = d < 1
- This implies that, for w ∈ D, |gn(w)| ≤ (d + ǫ)n, for large n.
- A wandering domain that is the lift of an attracting basin is
strongly contracting
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Contracting wandering domains
Recall U is contracting if ∞
n=0(1 − |g′ n(0)|) = ∞.
This implies that, for w ∈ D, gn(w) → 0 as n → ∞. U is strongly contracting if lim sup 1
n
n
k=1 |g′ k(0)| = d < 1
- This implies that, for w ∈ D, |gn(w)| ≤ (d + ǫ)n, for large n.
- A wandering domain that is the lift of an attracting basin is
strongly contracting
- A wandering domain that is the lift of a parabolic basin is
not strongly contracting.
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Contracting wandering domains
Recall U is contracting if ∞
n=0(1 − |g′ n(0)|) = ∞.
This implies that, for w ∈ D, gn(w) → 0 as n → ∞. U is strongly contracting if lim sup 1
n
n
k=1 |g′ k(0)| = d < 1
- This implies that, for w ∈ D, |gn(w)| ≤ (d + ǫ)n, for large n.
- A wandering domain that is the lift of an attracting basin is
strongly contracting
- A wandering domain that is the lift of a parabolic basin is
not strongly contracting.
U is super-contracting if lim 1
n
n
k=1 |g′ k(0)| = 0
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Contracting wandering domains
Recall U is contracting if ∞
n=0(1 − |g′ n(0)|) = ∞.
This implies that, for w ∈ D, gn(w) → 0 as n → ∞. U is strongly contracting if lim sup 1
n
n
k=1 |g′ k(0)| = d < 1
- This implies that, for w ∈ D, |gn(w)| ≤ (d + ǫ)n, for large n.
- A wandering domain that is the lift of an attracting basin is
strongly contracting
- A wandering domain that is the lift of a parabolic basin is
not strongly contracting.
U is super-contracting if lim 1
n
n
k=1 |g′ k(0)| = 0
- This implies that, for w ∈ D, d ∈ (0, 1), |gn(w)| ≤ dn, for
large n.
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Contracting wandering domains
Recall U is contracting if ∞
n=0(1 − |g′ n(0)|) = ∞.
This implies that, for w ∈ D, gn(w) → 0 as n → ∞. U is strongly contracting if lim sup 1
n
n
k=1 |g′ k(0)| = d < 1
- This implies that, for w ∈ D, |gn(w)| ≤ (d + ǫ)n, for large n.
- A wandering domain that is the lift of an attracting basin is
strongly contracting
- A wandering domain that is the lift of a parabolic basin is
not strongly contracting.
U is super-contracting if lim 1
n
n
k=1 |g′ k(0)| = 0
- This implies that, for w ∈ D, d ∈ (0, 1), |gn(w)| ≤ dn, for
large n.
- A wandering domain that is the lift of a super-attracting
basin is super-contracting.
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Classifying simply connected wandering domains
Distance from boundary
Theorem Let U be a simply connected wandering domain. Then there are three possibilities.
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Classifying simply connected wandering domains
Distance from boundary
Theorem Let U be a simply connected wandering domain. Then there are three possibilities. A Away For all z ∈ U, f n(z) stays away from ∂Un.
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Classifying simply connected wandering domains
Distance from boundary
Theorem Let U be a simply connected wandering domain. Then there are three possibilities. A Away For all z ∈ U, f n(z) stays away from ∂Un. B Bungee For all z ∈ U, there is a subsequence f nk(z) which converges to ∂Unk and a subsequence which stays away.
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Classifying simply connected wandering domains
Distance from boundary
Theorem Let U be a simply connected wandering domain. Then there are three possibilities. A Away For all z ∈ U, f n(z) stays away from ∂Un. B Bungee For all z ∈ U, there is a subsequence f nk(z) which converges to ∂Unk and a subsequence which stays away. C Converges For all z ∈ U, f n(z) converges to ∂Un.
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Classifying simply connected wandering domains
Distance from boundary
Theorem Let U be a simply connected wandering domain. Then there are three possibilities. A Away For all z ∈ U, f n(z) stays away from ∂Un. B Bungee For all z ∈ U, there is a subsequence f nk(z) which converges to ∂Unk and a subsequence which stays away. C Converges For all z ∈ U, f n(z) converges to ∂Un. Definition We say f n(z) converges to the boundary if ∆nρUn(f n(z)) → ∞ as n → ∞,
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Classifying simply connected wandering domains
Distance from boundary
Theorem Let U be a simply connected wandering domain. Then there are three possibilities. A Away For all z ∈ U, f n(z) stays away from ∂Un. B Bungee For all z ∈ U, there is a subsequence f nk(z) which converges to ∂Unk and a subsequence which stays away. C Converges For all z ∈ U, f n(z) converges to ∂Un. Definition We say f n(z) converges to the boundary if ∆nρUn(f n(z)) → ∞ as n → ∞, ∆n = sup{
d 1+d : d = diamD, D is a disc contained in Un}.
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Examples of simply connected wandering domains
These two theorems together give 9 classes of simply connected wandering domains.
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Examples of simply connected wandering domains
These two theorems together give 9 classes of simply connected wandering domains. All previously known examples of escaping wandering domains belong to just 3 of these classes.
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Examples of simply connected wandering domains
These two theorems together give 9 classes of simply connected wandering domains. All previously known examples of escaping wandering domains belong to just 3 of these classes. We give a new technique which allows us to construct examples of all 9 possible types of bounded escaping wandering domains.
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