Quantitative rectifiability in the Heisenberg group Katrin F assler - - PowerPoint PPT Presentation
Quantitative rectifiability in the Heisenberg group Katrin F assler - - PowerPoint PPT Presentation
Quantitative rectifiability in the Heisenberg group Katrin F assler University of Fribourg, Switzerland Joint work with Vasileios Chousionis and Tuomas Orponen Quantitative rectifiability in the Heisenberg group (of codimension 1 sets)
Quantitative rectifiability in the Heisenberg group
(of codimension 1 sets) Katrin F¨ assler University of Fribourg, Switzerland
Joint work with Vasileios Chousionis and Tuomas Orponen
The Heisenberg group
H1 = (R3, ∗) d(p, q) = q−1 ∗ p, where (x, y, t) = max{|(x, y)|, |t|1/2} The resulting space (H1, d) has Hausdorff dimension 4.
Rectifiability in H1
Rectifiability in H1
- L. Ambrosio and B. Kirchheim, 2000
Let k ≥ 2. If f : A ⊆ Rk → H1 is Lipschitz, then Hk(f (A)) = 0.
Rectifiability in H1
- L. Ambrosio and B. Kirchheim, 2000
Let k ≥ 2. If f : A ⊆ Rk → H1 is Lipschitz, then Hk(f (A)) = 0.
- B. Franchi, R. Serapioni, and F. Serra Cassano, 2001–. . .
In H1, consider an alternative to Federer’s definition of 3-rectifiability, for instance using intrinsic Lipschitz graphs.
Rectifiability in H1
- L. Ambrosio and B. Kirchheim, 2000
Let k ≥ 2. If f : A ⊆ Rk → H1 is Lipschitz, then Hk(f (A)) = 0.
- B. Franchi, R. Serapioni, and F. Serra Cassano, 2001–. . .
In H1, consider an alternative to Federer’s definition of 3-rectifiability, for instance using intrinsic Lipschitz graphs. Goal: study quantitative rectifiability in H1 (for codimension 1) (low dimensional sets: Franchi-Ferrari-Pajot, Juillet, Li-Schul, Hahlomaa) Motivation: uniform rectifiability in Rn (G. David and S. Semmes).
Towards the definition of intrinsic Lipschitz graphs
Write H1 = W ∗ V, where W - vertical 2-d subspace in R3, V - perpendicular 1-d horizontal subspace.
Towards the definition of intrinsic Lipschitz graphs
Write H1 = W ∗ V, where W - vertical 2-d subspace in R3, V - perpendicular 1-d horizontal subspace.
Heisenberg projections
Vertical projections: πW : H1 → W, p = pW ∗ pV → pW. Horizontal projections: πV : H1 → V, p = pW ∗ pV → pV.
Towards the definition of intrinsic Lipschitz graphs
Write H1 = W ∗ V, where W - vertical 2-d subspace in R3, V - perpendicular 1-d horizontal subspace.
Heisenberg projections
Vertical projections: πW : H1 → W, p = pW ∗ pV → pW. Horizontal projections: πV : H1 → V, p = pW ∗ pV → pV.
Heisenberg cone
CW(α) := {p ∈ H1 : πW(p) ≤ απV(p)}.
Intrinsic Lipschitz functions
Intrinsic L-Lipschitz graph
Γ ⊂ H1 such that (p ∗ CW( 1
L)) ∩ Γ = {p},
for all p ∈ Γ.
Intrinsic Lipschitz functions
Intrinsic L-Lipschitz graph
Γ ⊂ H1 such that (p ∗ CW( 1
L)) ∩ Γ = {p},
for all p ∈ Γ.
Intrinsic L-Lipschitz function
φ : A ⊆ W → V such that Γφ := {w ∗ φ(w) : w ∈ A} is an intrinsic L-Lipschitz graph. (φ is in general not metrically Lipschitz!)
The main result
Theorem
The following are equivalent for an Ahlfors 3-regular E ⊂ H1:
1 big pieces of intrinsic Lipschitz graphs 2 big vertical projections + weak geometric lemma for vertical β’s.
The main result
Theorem
The following are equivalent for an Ahlfors 3-regular E ⊂ H1:
1 big pieces of intrinsic Lipschitz graphs 2 big vertical projections + weak geometric lemma for vertical β’s.
big pieces of intrinsic Lipschitz graphs: ∃L ≥ 1, θ > 0: ∀x ∈ E, 0 < R ≤ diam(E) ∃Γ intrinsic L-Lipschitz: H3(E ∩ Γ ∩ B(x, R)) ≥ θR3.
The main result
Theorem
The following are equivalent for an Ahlfors 3-regular E ⊂ H1:
1 big pieces of intrinsic Lipschitz graphs 2 big vertical projections + weak geometric lemma for vertical β’s.
big pieces of intrinsic Lipschitz graphs: ∃L ≥ 1, θ > 0: ∀x ∈ E, 0 < R ≤ diam(E) ∃Γ intrinsic L-Lipschitz: H3(E ∩ Γ ∩ B(x, R)) ≥ θR3. big vertical projections: ∃δ > 0: ∀x ∈ E, 0 < R ≤ diamE ∃W vertical: L2(πW(E ∩ B(x, R))) ≥ δR3
The main result
Theorem
The following are equivalent for an Ahlfors 3-regular E ⊂ H1:
1 big pieces of intrinsic Lipschitz graphs 2 big vertical projections + weak geometric lemma for vertical β’s.
big pieces of intrinsic Lipschitz graphs: ∃L ≥ 1, θ > 0: ∀x ∈ E, 0 < R ≤ diam(E) ∃Γ intrinsic L-Lipschitz: H3(E ∩ Γ ∩ B(x, R)) ≥ θR3. big vertical projections: ∃δ > 0: ∀x ∈ E, 0 < R ≤ diamE ∃W vertical: L2(πW(E ∩ B(x, R))) ≥ δR3 vertical β-numbers: β(B) := infW,z supy∈B∩E
dist(y,z∗W) rad(B)
.
The main result
Theorem
The following are equivalent for an Ahlfors 3-regular E ⊂ H1:
1 big pieces of intrinsic Lipschitz graphs 2 big vertical projections + weak geometric lemma for vertical β’s.
big pieces of intrinsic Lipschitz graphs: ∃L ≥ 1, θ > 0: ∀x ∈ E, 0 < R ≤ diam(E) ∃Γ intrinsic L-Lipschitz: H3(E ∩ Γ ∩ B(x, R)) ≥ θR3. big vertical projections: ∃δ > 0: ∀x ∈ E, 0 < R ≤ diamE ∃W vertical: L2(πW(E ∩ B(x, R))) ≥ δR3 vertical β-numbers: β(B) := infW,z supy∈B∩E
dist(y,z∗W) rad(B)
. weak geometric lemma: ∀ε > 0, x ∈ E, R > 0 R
- E∩B(x,R)
χ{(y,s)∈E×R+: β(B(y,s))≥ε}(y, s)dH3(y)ds s ε R3.
Properties of intrinsic Lipschitz functions
- B. Franchi, R. Serapioni, F. Serra Cassano (2011); A. Naor, R. Young (2017) :
Properties of intrinsic L-Lipschitz φ : A ⊆ W → V
Properties of intrinsic Lipschitz functions
- B. Franchi, R. Serapioni, F. Serra Cassano (2011); A. Naor, R. Young (2017) :
Properties of intrinsic L-Lipschitz φ : A ⊆ W → V
p ∗ Γφ is intrinsic L-Lipschitz ∀p ∈ H1
Properties of intrinsic Lipschitz functions
- B. Franchi, R. Serapioni, F. Serra Cassano (2011); A. Naor, R. Young (2017) :
Properties of intrinsic L-Lipschitz φ : A ⊆ W → V
p ∗ Γφ is intrinsic L-Lipschitz ∀p ∈ H1 φ can be extended to an L′(L)-intrinsic Lipschitz function W → V
Properties of intrinsic Lipschitz functions
- B. Franchi, R. Serapioni, F. Serra Cassano (2011); A. Naor, R. Young (2017) :
Properties of intrinsic L-Lipschitz φ : A ⊆ W → V
p ∗ Γφ is intrinsic L-Lipschitz ∀p ∈ H1 φ can be extended to an L′(L)-intrinsic Lipschitz function W → V Γφ is Ahlfors-3-regular with constant depending on L (for A = W)
Properties of intrinsic Lipschitz functions
- B. Franchi, R. Serapioni, F. Serra Cassano (2011); A. Naor, R. Young (2017) :
Properties of intrinsic L-Lipschitz φ : A ⊆ W → V
p ∗ Γφ is intrinsic L-Lipschitz ∀p ∈ H1 φ can be extended to an L′(L)-intrinsic Lipschitz function W → V Γφ is Ahlfors-3-regular with constant depending on L (for A = W) φ is intrinsically differentiable in L2 a.e. w ∈ A, with intrinsic differential dφw : W → V, dφw(y, t) = ∇φφ(w)y, Intrinsically differentiable: (for φ(0) = 0) ∃dφ0 : W → V, intrinsic linear: |φ(y, t) − dφ0(y, t)| = o((y, t)); the general definition is by left-translation of the graph
Properties of intrinsic Lipschitz functions
- B. Franchi, R. Serapioni, F. Serra Cassano (2011); A. Naor, R. Young (2017) :
Properties of intrinsic L-Lipschitz φ : A ⊆ W → V
p ∗ Γφ is intrinsic L-Lipschitz ∀p ∈ H1 φ can be extended to an L′(L)-intrinsic Lipschitz function W → V Γφ is Ahlfors-3-regular with constant depending on L (for A = W) φ is intrinsically differentiable in L2 a.e. w ∈ A, with intrinsic differential dφw : W → V, dφw(y, t) = ∇φφ(w)y, φ has bounded intrinsic gradient ∇φφ∞ ≤ L
Properties of intrinsic Lipschitz functions
- B. Franchi, R. Serapioni, F. Serra Cassano (2011); A. Naor, R. Young (2017) :
Properties of intrinsic L-Lipschitz φ : A ⊆ W → V
p ∗ Γφ is intrinsic L-Lipschitz ∀p ∈ H1 φ can be extended to an L′(L)-intrinsic Lipschitz function W → V Γφ is Ahlfors-3-regular with constant depending on L (for A = W) φ is intrinsically differentiable in L2 a.e. w ∈ A, with intrinsic differential dφw : W → V, dφw(y, t) = ∇φφ(w)y, φ has bounded intrinsic gradient ∇φφ∞ ≤ L
Proof: Intrinsic Lipschitz graph ⇒ WGL
Let Γ = Γφ be the graph of an intrinsic Lipschitz function φ over W.
Proof: Intrinsic Lipschitz graph ⇒ WGL
Let Γ = Γφ be the graph of an intrinsic Lipschitz function φ over W.
First attempt to prove WGL for Γ
Γ ∩ B(y, s) is far from a vertical plane
?
⇒ gradient of φ fluctuates significantly in Γ ∩ B(y, s) ⇒ (with L∞ bound for gradient) WGL.
Proof: Intrinsic Lipschitz graph ⇒ WGL
Let Γ = Γφ be the graph of an intrinsic Lipschitz function φ over W.
First attempt to prove WGL for Γ
Γ ∩ B(y, s) is far from a vertical plane
?
⇒ gradient of φ fluctuates significantly in Γ ∩ B(y, s) ⇒ (with L∞ bound for gradient) WGL. This argument does not work for the intrinsic gradient!
Proof: Intrinsic Lipschitz graph ⇒ WGL
Let Γ = Γφ be the graph of an intrinsic Lipschitz function φ over W.
First attempt to prove WGL for Γ
Γ ∩ B(y, s) is far from a vertical plane
?
⇒ gradient of φ fluctuates significantly in Γ ∩ B(y, s) ⇒ (with L∞ bound for gradient) WGL. This argument does not work for the intrinsic gradient!
Example with ∇φφ(y, t) = ∂yφ(y, t) + φ(y, t)∂tφ(y, t) ≡ 0
Proof: Intrinsic Lipschitz graph ⇒ WGL
1 Property that forces ∇φφ to fluctuate a lot:
Γ being far from a intrinsic Lip constant gradient (CG) graph, (quantified by βCG-numbers)
Proof: Intrinsic Lipschitz graph ⇒ WGL
1 Property that forces ∇φφ to fluctuate a lot:
Γ being far from a intrinsic Lip constant gradient (CG) graph, (quantified by βCG-numbers)
2 ⇒ WGL for βCG (as before)
Proof: Intrinsic Lipschitz graph ⇒ WGL
1 Property that forces ∇φφ to fluctuate a lot:
Γ being far from a intrinsic Lip constant gradient (CG) graph, (quantified by βCG-numbers)
2 ⇒ WGL for βCG (as before) 3 globally defined intrinsic Lip CG graphs are (translated) vertical planes
Proof: Intrinsic Lipschitz graph ⇒ WGL
1 Property that forces ∇φφ to fluctuate a lot:
Γ being far from a intrinsic Lip constant gradient (CG) graph, (quantified by βCG-numbers)
2 ⇒ WGL for βCG (as before) 3 globally defined intrinsic Lip CG graphs are (translated) vertical planes 4 ⇒ (compactness argument)
CG graph defined in B(x, r) is almost flat in all sufficiently small sub-balls of B(x, r).
Proof: WGL and BVP ⇒ BPiLG
Proof: WGL and BVP ⇒ BPiLG
1 △ - David cubes on E. Define Q ∈ △ to be good if
β(Q) ≤ ε and L2(πW(Q)) ≥ cH3(Q).
Proof: WGL and BVP ⇒ BPiLG
1 △ - David cubes on E. Define Q ∈ △ to be good if
β(Q) ≤ ε and L2(πW(Q)) ≥ cH3(Q).
2 Geometric part:
(c, ε, W)-good Q ∈ △ is ‘almost’ intrinsic Lipschitz graph over W
Proof: WGL and BVP ⇒ BPiLG
1 △ - David cubes on E. Define Q ∈ △ to be good if
β(Q) ≤ ε and L2(πW(Q)) ≥ cH3(Q).
2 Geometric part:
(c, ε, W)-good Q ∈ △ is ‘almost’ intrinsic Lipschitz graph over W
3 Abstract part: modeled on David-Semmes “Quantitative rectifiability
and Lipschitz mappings” and Jones “Lipschitz and bi-Lipschitz functions”, but πW is not Lipschitz! However:
Proof: WGL and BVP ⇒ BPiLG
1 △ - David cubes on E. Define Q ∈ △ to be good if
β(Q) ≤ ε and L2(πW(Q)) ≥ cH3(Q).
2 Geometric part:
(c, ε, W)-good Q ∈ △ is ‘almost’ intrinsic Lipschitz graph over W
3 Abstract part: modeled on David-Semmes “Quantitative rectifiability
and Lipschitz mappings” and Jones “Lipschitz and bi-Lipschitz functions”, but πW is not Lipschitz! However:
Projection lemma
∃ 0 < C < ∞ such that for A ⊆ H1, one has L2(πW(A)) ≤ CH3(A).
Proof: WGL and BVP ⇒ BPiLG
1 △ - David cubes on E. Define Q ∈ △ to be good if
β(Q) ≤ ε and L2(πW(Q)) ≥ cH3(Q).
2 Geometric part:
(c, ε, W)-good Q ∈ △ is ‘almost’ intrinsic Lipschitz graph over W
3 Abstract part: modeled on David-Semmes “Quantitative rectifiability
and Lipschitz mappings” and Jones “Lipschitz and bi-Lipschitz functions”, but πW is not Lipschitz! However:
Projection lemma
∃ 0 < C < ∞ such that for A ⊆ H1, one has L2(πW(A)) ≤ CH3(A).
1
WGL, geometric part, and projection lemma ⇒ ∀Q0 ∈ △, W: ∃Fj ⊂ Q0 intrinsic L-Lipschitz: L2(πW(Q0 \ Fj)) ≤ bH3(Q0)
Proof: WGL and BVP ⇒ BPiLG
1 △ - David cubes on E. Define Q ∈ △ to be good if
β(Q) ≤ ε and L2(πW(Q)) ≥ cH3(Q).
2 Geometric part:
(c, ε, W)-good Q ∈ △ is ‘almost’ intrinsic Lipschitz graph over W
3 Abstract part: modeled on David-Semmes “Quantitative rectifiability
and Lipschitz mappings” and Jones “Lipschitz and bi-Lipschitz functions”, but πW is not Lipschitz! However:
Projection lemma
∃ 0 < C < ∞ such that for A ⊆ H1, one has L2(πW(A)) ≤ CH3(A).
1
WGL, geometric part, and projection lemma ⇒ ∀Q0 ∈ △, W: ∃Fj ⊂ Q0 intrinsic L-Lipschitz: L2(πW(Q0 \ Fj)) ≤ bH3(Q0)
2
BVP ⇒ ∃W, Q0 such that L2(πW(Q0)) ≥ 2bH3(Q0)
Proof: WGL and BVP ⇒ BPiLG
1 △ - David cubes on E. Define Q ∈ △ to be good if
β(Q) ≤ ε and L2(πW(Q)) ≥ cH3(Q).
2 Geometric part:
(c, ε, W)-good Q ∈ △ is ‘almost’ intrinsic Lipschitz graph over W
3 Abstract part: modeled on David-Semmes “Quantitative rectifiability
and Lipschitz mappings” and Jones “Lipschitz and bi-Lipschitz functions”, but πW is not Lipschitz! However:
Projection lemma
∃ 0 < C < ∞ such that for A ⊆ H1, one has L2(πW(A)) ≤ CH3(A).
1
WGL, geometric part, and projection lemma ⇒ ∀Q0 ∈ △, W: ∃Fj ⊂ Q0 intrinsic L-Lipschitz: L2(πW(Q0 \ Fj)) ≤ bH3(Q0)
2
BVP ⇒ ∃W, Q0 such that L2(πW(Q0)) ≥ 2bH3(Q0)
3