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A Non-Injective Skinning Map with a Critical Point Jonah Gaster - - PowerPoint PPT Presentation
A Non-Injective Skinning Map with a Critical Point Jonah Gaster - - PowerPoint PPT Presentation
A Non-Injective Skinning Map with a Critical Point Jonah Gaster University of Illinois - Chicago July 31, 2012 Introduction Introduction In his Geometrization for Haken 3-manifolds, Thurston described an inductive way to find hyperbolic
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Introduction
In his Geometrization for Haken 3-manifolds, Thurston described an inductive way to find hyperbolic structures on (irreducible, atoroidal) closed Haken 3-manifolds.
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Introduction
In his Geometrization for Haken 3-manifolds, Thurston described an inductive way to find hyperbolic structures on (irreducible, atoroidal) closed Haken 3-manifolds. He re-phrased the ”glueing problem” in terms of finding a fixed point of a certain holomorphic map on a Teichm¨ uller space.
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Introduction
In his Geometrization for Haken 3-manifolds, Thurston described an inductive way to find hyperbolic structures on (irreducible, atoroidal) closed Haken 3-manifolds. He re-phrased the ”glueing problem” in terms of finding a fixed point of a certain holomorphic map on a Teichm¨ uller space. Given a geometrically finite hyperbolic 3-manifold, M, with incompressible boundary Σ, the skinning map σM is a holomorphic map σM : T (Σ) → T (¯ Σ)
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Apart from Thurston’s insight, translating topological properties of M to dynamical properties of σM, little is known about the behaviour of skinning maps. Notable exceptions: The work of McMullen, Dumas and Kent.
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Apart from Thurston’s insight, translating topological properties of M to dynamical properties of σM, little is known about the behaviour of skinning maps. Notable exceptions: The work of McMullen, Dumas and Kent. Bounded Image Theorem (Thurston, 1979) If M is acylindrical, σM has compact image.
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Apart from Thurston’s insight, translating topological properties of M to dynamical properties of σM, little is known about the behaviour of skinning maps. Notable exceptions: The work of McMullen, Dumas and Kent. Bounded Image Theorem (Thurston, 1979) If M is acylindrical, σM has compact image. Theorem (McMullen, 1993): If M is acylindrical, dσM < c < 1.
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Apart from Thurston’s insight, translating topological properties of M to dynamical properties of σM, little is known about the behaviour of skinning maps. Notable exceptions: The work of McMullen, Dumas and Kent. Bounded Image Theorem (Thurston, 1979) If M is acylindrical, σM has compact image. Theorem (McMullen, 1993): If M is acylindrical, dσM < c < 1. Theorem (Kent, 2009): If M is acylindrical, diam(σM) is controlled by vol(M)
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Apart from Thurston’s insight, translating topological properties of M to dynamical properties of σM, little is known about the behaviour of skinning maps. Notable exceptions: The work of McMullen, Dumas and Kent. Bounded Image Theorem (Thurston, 1979) If M is acylindrical, σM has compact image. Theorem (McMullen, 1993): If M is acylindrical, dσM < c < 1. Theorem (Kent, 2009): If M is acylindrical, diam(σM) is controlled by vol(M) Theorem (Dumas, 2011): σM is open and finite-to-one.
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Question:
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Question:
◮ How nice is σM? Is it always an immersion? covering map?
diffeomorphism onto its image?
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Question:
◮ How nice is σM? Is it always an immersion? covering map?
diffeomorphism onto its image? We present a negative answer to the questions above: Theorem (G.): There exists a hyperbolic structure on a genus-2 handlebody, with two rank-1 cusps, whose skinning map is non-injective and has a critical point.
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Outline
Background Invariants of Quasi-Fuchsian and Geometrically Finite groups Pared 3-manifolds The skinning map σM and a useful lemma The definition A Symmetry Lemma The Example Glueing an Octahedron 4-Punctured Spheres The Path of Quasi-Fuchsian Groups Non-monotonicity Further Questions
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Background: 1. Kleinian Groups
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Background: 1. Kleinian Groups
◮ A Kleinian group Γ is a non-elementary, discrete, torsion-free
subgroup of PSL2(C).
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Background: 1. Kleinian Groups
◮ A Kleinian group Γ is a non-elementary, discrete, torsion-free
subgroup of PSL2(C).
◮ The limit set ΛΓ ⊂ CP1
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Background: 1. Kleinian Groups
◮ A Kleinian group Γ is a non-elementary, discrete, torsion-free
subgroup of PSL2(C).
◮ The limit set ΛΓ ⊂ CP1 ◮ The domain of discontinuity ΩΓ = CP1 \ ΛΓ
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Background: 1. Kleinian Groups
◮ A Kleinian group Γ is a non-elementary, discrete, torsion-free
subgroup of PSL2(C).
◮ The limit set ΛΓ ⊂ CP1 ◮ The domain of discontinuity ΩΓ = CP1 \ ΛΓ ◮ A quasi-Fuchsian group is a Kleinian group whose limit set is
a Jordan curve.
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Background: 1. Kleinian Groups
◮ A Kleinian group Γ is a non-elementary, discrete, torsion-free
subgroup of PSL2(C).
◮ The limit set ΛΓ ⊂ CP1 ◮ The domain of discontinuity ΩΓ = CP1 \ ΛΓ ◮ A quasi-Fuchsian group is a Kleinian group whose limit set is
a Jordan curve.
◮ A geometrically finite group is a Kleinian group possessing a
finite-sided polyhedral fundamental domain.
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Background: 1. Kleinian Groups
◮ A Kleinian group Γ is a non-elementary, discrete, torsion-free
subgroup of PSL2(C).
◮ The limit set ΛΓ ⊂ CP1 ◮ The domain of discontinuity ΩΓ = CP1 \ ΛΓ ◮ A quasi-Fuchsian group is a Kleinian group whose limit set is
a Jordan curve.
◮ A geometrically finite group is a Kleinian group possessing a
finite-sided polyhedral fundamental domain. Every hyperbolic 3-manifold is determined by the conjugacy class
- f a Kleinian group, so we may blur the distinction between Γ and
H3/Γ.
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Background: 2. Invariants of Kleinian Groups
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Background: 2. Invariants of Kleinian Groups
A geometrically finite Kleinian group Γ has several geometric invariants.
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Background: 2. Invariants of Kleinian Groups
A geometrically finite Kleinian group Γ has several geometric invariants.
◮ The convex hull of ΛΓ, CΓ ⊂ H3, and the convex core CΓ/Γ
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Background: 2. Invariants of Kleinian Groups
A geometrically finite Kleinian group Γ has several geometric invariants.
◮ The convex hull of ΛΓ, CΓ ⊂ H3, and the convex core CΓ/Γ ◮ The convex core boundary components (when non-empty),
”pleated” planes in H3, and the convex core boundary surfaces, their quotients under Γ
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Background: 2. Invariants of Kleinian Groups
A geometrically finite Kleinian group Γ has several geometric invariants.
◮ The convex hull of ΛΓ, CΓ ⊂ H3, and the convex core CΓ/Γ ◮ The convex core boundary components (when non-empty),
”pleated” planes in H3, and the convex core boundary surfaces, their quotients under Γ
◮ The bending laminations λΓ on the convex core boundary
surfaces (when non-empty)
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Background: 2. Invariants of Kleinian Groups
A geometrically finite Kleinian group Γ has several geometric invariants.
◮ The convex hull of ΛΓ, CΓ ⊂ H3, and the convex core CΓ/Γ ◮ The convex core boundary components (when non-empty),
”pleated” planes in H3, and the convex core boundary surfaces, their quotients under Γ
◮ The bending laminations λΓ on the convex core boundary
surfaces (when non-empty)
◮ The conformal boundary surfaces (when non-empty),
quotients of components of ΩΓ by Γ
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Background: 3. Quasi-Fuchsian vs. Geometrically Finite
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Background: 3. Quasi-Fuchsian vs. Geometrically Finite
Notation:
◮ QF(Σ) ⊂ Hom ( π1(Σ), PSL2(C) ) / PSL2(C) ◮ GF(M) ⊂ Hom ( π1(M), PSL2(C) ) / PSL2(C)
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Background: 3. Quasi-Fuchsian vs. Geometrically Finite
Notation:
◮ QF(Σ) ⊂ Hom ( π1(Σ), PSL2(C) ) / PSL2(C) ◮ GF(M) ⊂ Hom ( π1(M), PSL2(C) ) / PSL2(C)
Important Fact If Ω0 is a component of Ωˆ
Γ, ˆ
Γ a geometrically finite Kleinian group, then Stab(Ω0) is quasi-Fuchsian.
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Background: 3. Quasi-Fuchsian vs. Geometrically Finite
Notation:
◮ QF(Σ) ⊂ Hom ( π1(Σ), PSL2(C) ) / PSL2(C) ◮ GF(M) ⊂ Hom ( π1(M), PSL2(C) ) / PSL2(C)
Important Fact If Ω0 is a component of Ωˆ
Γ, ˆ
Γ a geometrically finite Kleinian group, then Stab(Ω0) is quasi-Fuchsian. This Important Fact (IF) will make a couple of appearances. The proof uses 3-manifold topology.
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Background: 4. The Cartoon of a Quasi-Fuchsian Group
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Background: 4. The Cartoon of a Quasi-Fuchsian Group
The quasiconformal deformation theory developed by Ahlfors and Bers allows the following simple characterization:
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Background: 4. The Cartoon of a Quasi-Fuchsian Group
The quasiconformal deformation theory developed by Ahlfors and Bers allows the following simple characterization: Bers’ Simultaneous Uniformization QF(Σ) ∼ = T (Σ) × T (¯ Σ)
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Background: 4. The Cartoon of a Quasi-Fuchsian Group
The quasiconformal deformation theory developed by Ahlfors and Bers allows the following simple characterization: Bers’ Simultaneous Uniformization QF(Σ) ∼ = T (Σ) × T (¯ Σ) The geomeric invariants of a quasi-Fuchsian group can be grouped into a convenient cartoon.
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Background: 5. Pared 3-manifolds
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Background: 5. Pared 3-manifolds
A careful treatment of geometrically finite hyperbolic structures on 3-manifolds with cusps requires the discussion of pared manifolds.
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Background: 5. Pared 3-manifolds
A careful treatment of geometrically finite hyperbolic structures on 3-manifolds with cusps requires the discussion of pared manifolds. For pared manifold M = (M0, P):
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Background: 5. Pared 3-manifolds
A careful treatment of geometrically finite hyperbolic structures on 3-manifolds with cusps requires the discussion of pared manifolds. For pared manifold M = (M0, P):
◮ M0 is a compact 3-manifold with boundary
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Background: 5. Pared 3-manifolds
A careful treatment of geometrically finite hyperbolic structures on 3-manifolds with cusps requires the discussion of pared manifolds. For pared manifold M = (M0, P):
◮ M0 is a compact 3-manifold with boundary ◮ P ⊂ ∂M0 is a disjoint union of incompressible tori and annuli
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Background: 5. Pared 3-manifolds
A careful treatment of geometrically finite hyperbolic structures on 3-manifolds with cusps requires the discussion of pared manifolds. For pared manifold M = (M0, P):
◮ M0 is a compact 3-manifold with boundary ◮ P ⊂ ∂M0 is a disjoint union of incompressible tori and annuli ◮ ∂M = ⊔iΣi denotes ∂M0 \ ∂P
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Background: 5. Pared 3-manifolds
A careful treatment of geometrically finite hyperbolic structures on 3-manifolds with cusps requires the discussion of pared manifolds. For pared manifold M = (M0, P):
◮ M0 is a compact 3-manifold with boundary ◮ P ⊂ ∂M0 is a disjoint union of incompressible tori and annuli ◮ ∂M = ⊔iΣi denotes ∂M0 \ ∂P
GF(M) = {[ρ] ∈ GF(M0) | ρ(γ) is parabolic ⇔ γ ∈ π1(P)}
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Background: 5. Pared 3-manifolds
A careful treatment of geometrically finite hyperbolic structures on 3-manifolds with cusps requires the discussion of pared manifolds. For pared manifold M = (M0, P):
◮ M0 is a compact 3-manifold with boundary ◮ P ⊂ ∂M0 is a disjoint union of incompressible tori and annuli ◮ ∂M = ⊔iΣi denotes ∂M0 \ ∂P
GF(M) = {[ρ] ∈ GF(M0) | ρ(γ) is parabolic ⇔ γ ∈ π1(P)} Theorem (Ahlfors, Bers, Marden, Sullivan) GF(M) ∼ =
i T (Σi)
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Background: Review
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Background: Review
Most important things to keep in mind:
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Background: Review
Most important things to keep in mind:
◮ The cartoon of a quasi-Fuchsian 3-manifold
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Background: Review
Most important things to keep in mind:
◮ The cartoon of a quasi-Fuchsian 3-manifold ◮ QF(Σ) ∼
= T (Σ) × T (¯ Σ)
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Background: Review
Most important things to keep in mind:
◮ The cartoon of a quasi-Fuchsian 3-manifold ◮ QF(Σ) ∼
= T (Σ) × T (¯ Σ)
◮ GF(M) ∼
=
i T (Σi)
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Background: Review
Most important things to keep in mind:
◮ The cartoon of a quasi-Fuchsian 3-manifold ◮ QF(Σ) ∼
= T (Σ) × T (¯ Σ)
◮ GF(M) ∼
=
i T (Σi) ◮ The IF: Stab(Ωi) < ˆ
Γ is quasi-Fuchsian
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The Definition
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The Definition
In everything that follows, M = (M0, P) is a geometrically finite pared 3-manifold with incompressible boundary Σ = ∂M = ⊔iΣi.
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The Definition
In everything that follows, M = (M0, P) is a geometrically finite pared 3-manifold with incompressible boundary Σ = ∂M = ⊔iΣi. The inclusion π1(Σi) ֒ → π1(M) induces the restriction map ri on (conjugacy classes of) representations.
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The Definition
In everything that follows, M = (M0, P) is a geometrically finite pared 3-manifold with incompressible boundary Σ = ∂M = ⊔iΣi. The inclusion π1(Σi) ֒ → π1(M) induces the restriction map ri on (conjugacy classes of) representations. Definition The skinning map σM is given by
- i T (Σi)
σi
M
- ∼
=
GF(M)
ri
QF(Σi)
∼ =
T (Σi) × T ( ¯
Σi)
p2
- T ( ¯
Σi) σM =
i σi M : i T (Σi) → i T ( ¯
Σi)
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The Definition
In everything that follows, M = (M0, P) is a geometrically finite pared 3-manifold with incompressible boundary Σ = ∂M = ⊔iΣi. The inclusion π1(Σi) ֒ → π1(M) induces the restriction map ri on (conjugacy classes of) representations. Definition The skinning map σM is given by
- i T (Σi)
σi
M
- ∼
=
GF(M)
ri
QF(Σi)
∼ =
T (Σi) × T ( ¯
Σi)
p2
- T ( ¯
Σi) σM =
i σi M : i T (Σi) → i T ( ¯
Σi) ri lands in QF(Σi) because of the IF.
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Background: The Definition, Again
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Background: The Definition, Again
Assume for simplicity that M has only one boundary component.
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Background: The Definition, Again
Assume for simplicity that M has only one boundary component. The cover of M corresponding to π1(Σ) < π1(M):
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Background: The Definition, Again
Assume for simplicity that M has only one boundary component. The cover of M corresponding to π1(Σ) < π1(M):
X X σM (X ) M
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Background: The Definition, Again
Assume for simplicity that M has only one boundary component. The cover of M corresponding to π1(Σ) < π1(M):
X X σM (X ) M
IF - The cover is quasi-Fuchsian
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Background: The Definition, Again
Assume for simplicity that M has only one boundary component. The cover of M corresponding to π1(Σ) < π1(M):
X X σM (X ) M
IF - The cover is quasi-Fuchsian Note that σM depends only on the topology of (M, Σ).
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Background: A Simple Example
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Background: A Simple Example
Suppose M is quasi-Fuchsian. That is, M ∼ = H3/Γ, for Γ < PSL2(C) quasi-Fuchsian. Topologically, M ∼ = Σ × [0, 1].
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Background: A Simple Example
Suppose M is quasi-Fuchsian. That is, M ∼ = H3/Γ, for Γ < PSL2(C) quasi-Fuchsian. Topologically, M ∼ = Σ × [0, 1]. Then ∂M ∼ = Σ ⊔ ¯ Σ, so T (∂M) ∼ = T (Σ) × T (¯ Σ)
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Background: A Simple Example
Suppose M is quasi-Fuchsian. That is, M ∼ = H3/Γ, for Γ < PSL2(C) quasi-Fuchsian. Topologically, M ∼ = Σ × [0, 1]. Then ∂M ∼ = Σ ⊔ ¯ Σ, so T (∂M) ∼ = T (Σ) × T (¯ Σ) In this case, σM(X, ¯ Y ) = ( ¯ Y , X)
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A Symmetry Lemma
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A Symmetry Lemma
Let M = (M0, P) is a geometrically finite pared 3-manifold with incompressible boundary Σ.
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A Symmetry Lemma
Let M = (M0, P) is a geometrically finite pared 3-manifold with incompressible boundary Σ. Supposeφ ∈ Diff(M0) satisfies φ(P) = P. Then φ induces Φ ∈ MCG∗(M) ⊂ MCG∗(Σ). In this case,
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A Symmetry Lemma
Let M = (M0, P) is a geometrically finite pared 3-manifold with incompressible boundary Σ. Supposeφ ∈ Diff(M0) satisfies φ(P) = P. Then φ induces Φ ∈ MCG∗(M) ⊂ MCG∗(Σ). In this case, Symmetry Lemma σM (Fix Φ) ⊂ Fix Φ
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A Symmetry Lemma
Let M = (M0, P) is a geometrically finite pared 3-manifold with incompressible boundary Σ. Supposeφ ∈ Diff(M0) satisfies φ(P) = P. Then φ induces Φ ∈ MCG∗(M) ⊂ MCG∗(Σ). In this case, Symmetry Lemma σM (Fix Φ) ⊂ Fix Φ This lemma is an immediate consequence of the observation that σM is MCG∗(M)-equivariant.
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Strategy
Strategy Use the Symmetry Lemma to cut down dimensions and complexity, making σM accessible.
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Strategy
Strategy Use the Symmetry Lemma to cut down dimensions and complexity, making σM accessible. In the example that follows, T (Σ) ∼ = H, so σM is ’only’ a holomorphic map H → H.
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Strategy
Strategy Use the Symmetry Lemma to cut down dimensions and complexity, making σM accessible. In the example that follows, T (Σ) ∼ = H, so σM is ’only’ a holomorphic map H → H. Non-monotonicity restricted to a real one-dimensional submanifold guarantees the existence of a critical point.
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The Example: Glueing an Octahedron
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The Example: Glueing an Octahedron
Glue the green faces of the octahedron, in pairs, with twists:
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The Example: Glueing an Octahedron
Glue the green faces of the octahedron, in pairs, with twists:
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The Example: Glueing an Octahedron
Glue the green faces of the octahedron, in pairs, with twists:
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The Example: Glueing an Octahedron
Glue the green faces of the octahedron, in pairs, with twists:
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The Pared Manifold
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The Pared Manifold
In the resulting pared 3-manifold M = (M0, P), M◦ is a genus 2 handlebody, and P consists of (annuli neighborhoods of) 2 essential curves in ∂M0.
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The Pared Manifold
In the resulting pared 3-manifold M = (M0, P), M◦ is a genus 2 handlebody, and P consists of (annuli neighborhoods of) 2 essential curves in ∂M0. The curves in P are disk-busting, so by a Lemma of Otal, M is acylindrical and Σ = ∂M is incompressible.
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The Pared Manifold
In the resulting pared 3-manifold M = (M0, P), M◦ is a genus 2 handlebody, and P consists of (annuli neighborhoods of) 2 essential curves in ∂M0. The curves in P are disk-busting, so by a Lemma of Otal, M is acylindrical and Σ = ∂M is incompressible. The boundary Σ is a four-holed sphere.
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A Path in GF(M)
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A Path in GF(M)
Consider the regular ideal octahedron in H3, with vertices {0, ±1, ±i, ∞}, and perform the indicated face identifications with M¨
- bius transformations. This determines a representation
ρ1 : π1(M) → PSL2(C).
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A Path in GF(M)
Consider the regular ideal octahedron in H3, with vertices {0, ±1, ±i, ∞}, and perform the indicated face identifications with M¨
- bius transformations. This determines a representation
ρ1 : π1(M) → PSL2(C). One may check:
◮ ρ1(π1(P)) is purely parabolic
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A Path in GF(M)
Consider the regular ideal octahedron in H3, with vertices {0, ±1, ±i, ∞}, and perform the indicated face identifications with M¨
- bius transformations. This determines a representation
ρ1 : π1(M) → PSL2(C). One may check:
◮ ρ1(π1(P)) is purely parabolic ◮ ρ1(π1(Σ)) is Fuchsian
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A Path in GF(M)
Consider the regular ideal octahedron in H3, with vertices {0, ±1, ±i, ∞}, and perform the indicated face identifications with M¨
- bius transformations. This determines a representation
ρ1 : π1(M) → PSL2(C). One may check:
◮ ρ1(π1(P)) is purely parabolic ◮ ρ1(π1(Σ)) is Fuchsian ◮ ρ1 ∈ GF(M)
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A Path in GF(M)
Consider the regular ideal octahedron in H3, with vertices {0, ±1, ±i, ∞}, and perform the indicated face identifications with M¨
- bius transformations. This determines a representation
ρ1 : π1(M) → PSL2(C). One may check:
◮ ρ1(π1(P)) is purely parabolic ◮ ρ1(π1(Σ)) is Fuchsian ◮ ρ1 ∈ GF(M)
Since geometric finiteness is an open condition, we can deform the representation ρ1 in GF(M). Let ρt indicate the same face identifications, for the octahedron with vertices {0, ±1, ±it, ∞}.
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A Path in GF(M)
Consider the regular ideal octahedron in H3, with vertices {0, ±1, ±i, ∞}, and perform the indicated face identifications with M¨
- bius transformations. This determines a representation
ρ1 : π1(M) → PSL2(C). One may check:
◮ ρ1(π1(P)) is purely parabolic ◮ ρ1(π1(Σ)) is Fuchsian ◮ ρ1 ∈ GF(M)
Since geometric finiteness is an open condition, we can deform the representation ρ1 in GF(M). Let ρt indicate the same face identifications, for the octahedron with vertices {0, ±1, ±it, ∞}. Let Γt = ρt (π1(Σ)).
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’Rhombic’ Symmetry
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’Rhombic’ Symmetry
There is an order 4 orientation-reversing diffeomorphism of the genus 2 handlebody, that preserves P, and thus descends to a mapping class Φ ∈ MCG∗(Σ).
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’Rhombic’ Symmetry
There is an order 4 orientation-reversing diffeomorphism of the genus 2 handlebody, that preserves P, and thus descends to a mapping class Φ ∈ MCG∗(Σ). In fact, there are two curves ξ, η ∈ π1(Σ) preserved by Φ.
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’Rhombic’ Symmetry
There is an order 4 orientation-reversing diffeomorphism of the genus 2 handlebody, that preserves P, and thus descends to a mapping class Φ ∈ MCG∗(Σ). In fact, there are two curves ξ, η ∈ π1(Σ) preserved by Φ. By the Symmetry Lemma, the subset Fix Φ is preserved by σM.
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’Rhombic’ Symmetry
There is an order 4 orientation-reversing diffeomorphism of the genus 2 handlebody, that preserves P, and thus descends to a mapping class Φ ∈ MCG∗(Σ). In fact, there are two curves ξ, η ∈ π1(Σ) preserved by Φ. By the Symmetry Lemma, the subset Fix Φ is preserved by σM. One may check that Φ has a realization as a hyperbolic isometry normalizing Γt, i.e. [ρt] ∈ Fix Φ.
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’Rhombic’ Symmetry
There is an order 4 orientation-reversing diffeomorphism of the genus 2 handlebody, that preserves P, and thus descends to a mapping class Φ ∈ MCG∗(Σ). In fact, there are two curves ξ, η ∈ π1(Σ) preserved by Φ. By the Symmetry Lemma, the subset Fix Φ is preserved by σM. One may check that Φ has a realization as a hyperbolic isometry normalizing Γt, i.e. [ρt] ∈ Fix Φ. Question What is Fix Φ in T (Σ)?
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A Detour: 4-Punctued Spheres
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A Detour: 4-Punctued Spheres
Definition Φ ∈ MCG∗(Σ) is {ξ, η}-rhombic if it is order-4, orientation- reversing, and preserves simple closed curves ξ and η.
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A Detour: 4-Punctued Spheres
Definition Φ ∈ MCG∗(Σ) is {ξ, η}-rhombic if it is order-4, orientation- reversing, and preserves simple closed curves ξ and η. X ∈ T (Σ) is {ξ, η}-rhombic if X ∈ Fix Φ, for {ξ, η}-rhombic Φ.
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A Detour: 4-Punctued Spheres
Definition Φ ∈ MCG∗(Σ) is {ξ, η}-rhombic if it is order-4, orientation- reversing, and preserves simple closed curves ξ and η. X ∈ T (Σ) is {ξ, η}-rhombic if X ∈ Fix Φ, for {ξ, η}-rhombic Φ. Important facts about rhombic 4-punctured spheres:
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A Detour: 4-Punctued Spheres
Definition Φ ∈ MCG∗(Σ) is {ξ, η}-rhombic if it is order-4, orientation- reversing, and preserves simple closed curves ξ and η. X ∈ T (Σ) is {ξ, η}-rhombic if X ∈ Fix Φ, for {ξ, η}-rhombic Φ. Important facts about rhombic 4-punctured spheres:
◮ X can be formed by gluing isometric Euclidean rhombi
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A Detour: 4-Punctued Spheres
Definition Φ ∈ MCG∗(Σ) is {ξ, η}-rhombic if it is order-4, orientation- reversing, and preserves simple closed curves ξ and η. X ∈ T (Σ) is {ξ, η}-rhombic if X ∈ Fix Φ, for {ξ, η}-rhombic Φ. Important facts about rhombic 4-punctured spheres:
◮ X can be formed by gluing isometric Euclidean rhombi ◮ Fix Φ = {ξ, η} ⊂ ML(Σ)
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A Detour: 4-Punctued Spheres
Definition Φ ∈ MCG∗(Σ) is {ξ, η}-rhombic if it is order-4, orientation- reversing, and preserves simple closed curves ξ and η. X ∈ T (Σ) is {ξ, η}-rhombic if X ∈ Fix Φ, for {ξ, η}-rhombic Φ. Important facts about rhombic 4-punctured spheres:
◮ X can be formed by gluing isometric Euclidean rhombi ◮ Fix Φ = {ξ, η} ⊂ ML(Σ) ◮ Ext(ξ, ·), Ext(η, ·), ℓ(ξ, ·), and ℓ(η, ·) each provide
diffeomorphisms from {X| X is {ξ, η}-rhombic} to R+
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A Detour: 4-Punctued Spheres
Definition Φ ∈ MCG∗(Σ) is {ξ, η}-rhombic if it is order-4, orientation- reversing, and preserves simple closed curves ξ and η. X ∈ T (Σ) is {ξ, η}-rhombic if X ∈ Fix Φ, for {ξ, η}-rhombic Φ. Important facts about rhombic 4-punctured spheres:
◮ X can be formed by gluing isometric Euclidean rhombi ◮ Fix Φ = {ξ, η} ⊂ ML(Σ) ◮ Ext(ξ, ·), Ext(η, ·), ℓ(ξ, ·), and ℓ(η, ·) each provide
diffeomorphisms from {X| X is {ξ, η}-rhombic} to R+
◮ Ext(ξ, X) = 4Mod(QX), where Q is the quotient of X by its
two orientation-reversing involutions
SLIDE 103
The Path of Quasi-Fuchsian Groups
SLIDE 104
The Path of Quasi-Fuchsian Groups
Lemma For t ∈ (t0, 1], Γt is quasi-Fuchsian, with bending lamination on bottom (resp. top) given by θt · ξ (resp. ϑt · η), and convex core boundary surface on bottom (resp. top) determined by ℓt = ℓ(ξ, ρt) (resp. ℓ(η, ρt)). t0, θt, and ℓt are all explicit.
SLIDE 105
The Path of Quasi-Fuchsian Groups
Lemma For t ∈ (t0, 1], Γt is quasi-Fuchsian, with bending lamination on bottom (resp. top) given by θt · ξ (resp. ϑt · η), and convex core boundary surface on bottom (resp. top) determined by ℓt = ℓ(ξ, ρt) (resp. ℓ(η, ρt)). t0, θt, and ℓt are all explicit. Crucial step: Since Γt is preserved by the rhombic symmetry Φ, all
- f its geometric invariants are also. This ensures that the bending
laminations are contained in the set {ξ, η}.
SLIDE 106
Background Again: Grafting
SLIDE 107
Background Again: Grafting
Problem How do we go from the convex core boundary to the conformal boundary?
SLIDE 108
Background Again: Grafting
Problem How do we go from the convex core boundary to the conformal boundary?
Solution:
Grafting provides a geometric way of passing back and forth between the convex core boundary, with its bending lamination, and the conformal boundary: gr : ML(Σ) × T (Σ) → T (Σ)
SLIDE 109
Parameterizing the Image
Qt θ
t
X t γ ξ
SLIDE 110
Parameterizing the Image
Now we can build a projective model for the surface in the image, at every point along our deformation path:
Qt θ
t
X t γ ξ
SLIDE 111
Parameterizing the Image
Now we can build a projective model for the surface in the image, at every point along our deformation path:
Qt θ
t
X t γ ξ
Xt is gr (θt · ξ, Yt), where Yt is the {ξ, η}-rhombic 4-punctured sphere determined by ℓ(ξ, Γt).
SLIDE 112
Non-monotonicity
SLIDE 113
Non-monotonicity
Recall:
SLIDE 114
Non-monotonicity
Recall:
◮ Ext(ξ, ·) parameterizes the {ξ, η}-rhombic set in T (Σ)
SLIDE 115
Non-monotonicity
Recall:
◮ Ext(ξ, ·) parameterizes the {ξ, η}-rhombic set in T (Σ) ◮ Ext(ξ, Xt) = 4Mod(Qt)
SLIDE 116
Non-monotonicity
Recall:
◮ Ext(ξ, ·) parameterizes the {ξ, η}-rhombic set in T (Σ) ◮ Ext(ξ, Xt) = 4Mod(Qt)
For non-monotonicity of σM, it suffices to show non-monotonicity
- f Mod(Qt)
SLIDE 117
Non-monotonicity
Recall:
◮ Ext(ξ, ·) parameterizes the {ξ, η}-rhombic set in T (Σ) ◮ Ext(ξ, Xt) = 4Mod(Qt)
For non-monotonicity of σM, it suffices to show non-monotonicity
- f Mod(Qt)
Explicit estimates on moduli of quadrilaterals are surprisingly hard, especially when the quadrilateral has an ideal vertex. Fortunately, a normalizing map will make a comparison accessible.
SLIDE 118
A Normalization for Qt
SLIDE 119
A Normalization for Qt
We normalize by sending a pair of sides into the vertical lines {ℜ(z) = 0} and {ℜ(z) = 1}.
SLIDE 120
A Normalization for Qt
We normalize by sending a pair of sides into the vertical lines {ℜ(z) = 0} and {ℜ(z) = 1}.
4 ℓt (log z − i π+θt 2 )
SLIDE 121
Finishing Non-monotonicity
SLIDE 122
Finishing Non-monotonicity
In these coordinates, the non-monotonicity becomes visually transparent, and, more importantly, possible to show explicitly!
SLIDE 123
Finishing Non-monotonicity
In these coordinates, the non-monotonicity becomes visually transparent, and, more importantly, possible to show explicitly!
SLIDE 124
Further Questions
SLIDE 125
Further Questions
Some natural problems:
SLIDE 126
Further Questions
Some natural problems:
◮ What is the critical point? An explanation of the geometric
role of the symmetry?
SLIDE 127