higher integrability of the harmonic measure [0.1cm] and ... · pdf filehigher integrability...
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![Page 1: Higher integrability of the Harmonic Measure [0.1cm] and ... · PDF fileHigher integrability of the Harmonic Measure and Uniform Recti ability Jos e Mar a Martell joint work with S](https://reader034.vdocuments.us/reader034/viewer/2022051720/5a78b15d7f8b9a852c8e9467/html5/thumbnails/1.jpg)
Higher integrability of the Harmonic Measure
and Uniform Rectifiability
Jose Marıa Martelljoint work with
S. Hofmann and with S. Hofmann, I. Uriarte-Tuero
Instituto de Ciencias MatematicasCSIC-UAM-UC3M-UCM
Spain
Conference in Harmonic Analysisand Partial Differential Equations
in honour of Eric Sawyer
Toronto, July 26–29, 2011
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Introduction Main results Strategy of the Proof
Section 1
Introduction
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 2 / 23
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Introduction Main results Strategy of the Proof
Introduction
Theorem (F. & M. Riesz 1916)
Ω ⊂ C simply connected domain with rectifiable boundary
harmonic measure ω σ = H1∣∣∂Ω
[Lavrentiev 1936] Quantitative version
[Bishop-Jones 1990]
E ⊂ ∂Ω, E rectifiable =⇒ ω σ on E
Counterexample F. & M. Riesz can fail without some topology
Goal: Obtain higher dimensional, scale-invariant (quantitative)version of F. & M. Riesz
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 3 / 23
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Introduction Main results Strategy of the Proof
Introduction
Theorem (F. & M. Riesz 1916)
Ω ⊂ C simply connected domain with rectifiable boundary
harmonic measure ω σ = H1∣∣∂Ω
[Lavrentiev 1936] Quantitative version
[Bishop-Jones 1990]
E ⊂ ∂Ω, E rectifiable =⇒ ω σ on E
Counterexample F. & M. Riesz can fail without some topology
Goal: Obtain higher dimensional, scale-invariant (quantitative)version of F. & M. Riesz
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 3 / 23
![Page 5: Higher integrability of the Harmonic Measure [0.1cm] and ... · PDF fileHigher integrability of the Harmonic Measure and Uniform Recti ability Jos e Mar a Martell joint work with S](https://reader034.vdocuments.us/reader034/viewer/2022051720/5a78b15d7f8b9a852c8e9467/html5/thumbnails/5.jpg)
Introduction Main results Strategy of the Proof
Introduction
Theorem (F. & M. Riesz 1916)
Ω ⊂ C simply connected domain with rectifiable boundary
harmonic measure ω σ = H1∣∣∂Ω
[Lavrentiev 1936] Quantitative version
[Bishop-Jones 1990]
E ⊂ ∂Ω, E rectifiable =⇒ ω σ on E
Counterexample F. & M. Riesz can fail without some topology
Goal: Obtain higher dimensional, scale-invariant (quantitative)version of F. & M. Riesz
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 3 / 23
![Page 6: Higher integrability of the Harmonic Measure [0.1cm] and ... · PDF fileHigher integrability of the Harmonic Measure and Uniform Recti ability Jos e Mar a Martell joint work with S](https://reader034.vdocuments.us/reader034/viewer/2022051720/5a78b15d7f8b9a852c8e9467/html5/thumbnails/6.jpg)
Introduction Main results Strategy of the Proof
Introduction
Theorem (F. & M. Riesz 1916)
Ω ⊂ C simply connected domain with rectifiable boundary
harmonic measure ω σ = H1∣∣∂Ω
[Lavrentiev 1936] Quantitative version
[Bishop-Jones 1990]
E ⊂ ∂Ω, E rectifiable =⇒ ω σ on E
Counterexample F. & M. Riesz can fail without some topology
Goal: Obtain higher dimensional, scale-invariant (quantitative)version of F. & M. Riesz
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 3 / 23
![Page 7: Higher integrability of the Harmonic Measure [0.1cm] and ... · PDF fileHigher integrability of the Harmonic Measure and Uniform Recti ability Jos e Mar a Martell joint work with S](https://reader034.vdocuments.us/reader034/viewer/2022051720/5a78b15d7f8b9a852c8e9467/html5/thumbnails/7.jpg)
Introduction Main results Strategy of the Proof
Harmonic measure
Ω ⊂ Rn+1, n ≥ 2, connected and open σ = Hn∣∣∂Ω
Surface ball ∆(x, r) = B(x, r) ∩ ∂Ω with x ∈ ∂Ω
Harmonic measure ωXX∈Ω family of probabilities on ∂Ω
u(X) =
∫∂Ωf(x) dωX(x) solves (D)
Lu = 0 in Ω
u∣∣∂Ω
= f ∈ Cc(∂Ω)
r
B
∆FωX
(F )
X
∂Ω
Ω
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 4 / 23
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Introduction Main results Strategy of the Proof
Harmonic measure
Ω ⊂ Rn+1, n ≥ 2, connected and open σ = Hn∣∣∂Ω
Surface ball ∆(x, r) = B(x, r) ∩ ∂Ω with x ∈ ∂Ω
Harmonic measure ωXX∈Ω family of probabilities on ∂Ω
u(X) =
∫∂Ωf(x) dωX(x) solves (D)
Lu = 0 in Ω
u∣∣∂Ω
= f ∈ Cc(∂Ω)
r
B
∆
FωX
(F )
X
∂Ω
Ω
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 4 / 23
![Page 9: Higher integrability of the Harmonic Measure [0.1cm] and ... · PDF fileHigher integrability of the Harmonic Measure and Uniform Recti ability Jos e Mar a Martell joint work with S](https://reader034.vdocuments.us/reader034/viewer/2022051720/5a78b15d7f8b9a852c8e9467/html5/thumbnails/9.jpg)
Introduction Main results Strategy of the Proof
Harmonic measure
Ω ⊂ Rn+1, n ≥ 2, connected and open σ = Hn∣∣∂Ω
Surface ball ∆(x, r) = B(x, r) ∩ ∂Ω with x ∈ ∂Ω
Harmonic measure ωXX∈Ω family of probabilities on ∂Ω
u(X) =
∫∂Ωf(x) dωX(x) solves (D)
Lu = 0 in Ω
u∣∣∂Ω
= f ∈ Cc(∂Ω)
r
B
∆FωX
(F )
X
∂Ω
Ω
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 4 / 23
![Page 10: Higher integrability of the Harmonic Measure [0.1cm] and ... · PDF fileHigher integrability of the Harmonic Measure and Uniform Recti ability Jos e Mar a Martell joint work with S](https://reader034.vdocuments.us/reader034/viewer/2022051720/5a78b15d7f8b9a852c8e9467/html5/thumbnails/10.jpg)
Introduction Main results Strategy of the Proof
Harmonic measure
Ω ⊂ Rn+1, n ≥ 2, connected and open σ = Hn∣∣∂Ω
Surface ball ∆(x, r) = B(x, r) ∩ ∂Ω with x ∈ ∂Ω
Harmonic measure ωXX∈Ω family of probabilities on ∂Ω
u(X) =
∫∂Ωf(x) dωX(x) solves (D)
Lu = 0 in Ω
u∣∣∂Ω
= f ∈ Cc(∂Ω)
r
B
∆
FωX
(F )
X
∂Ω
Ω
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 4 / 23
![Page 11: Higher integrability of the Harmonic Measure [0.1cm] and ... · PDF fileHigher integrability of the Harmonic Measure and Uniform Recti ability Jos e Mar a Martell joint work with S](https://reader034.vdocuments.us/reader034/viewer/2022051720/5a78b15d7f8b9a852c8e9467/html5/thumbnails/11.jpg)
Introduction Main results Strategy of the Proof
Qualitative vs. Quantitative (scale-invariant)
ω σ ω ∈ A∞(σ)
σ(F ) = 0 ⇒ ω(F ) = 0ω(F )
ω(∆).
(σ(F )
σ(∆)
)θ, F ⊂ ∆
Rectifiability Uniform rectifiability
r B∆
crX∆
∂Ω
Ω
No corkscrew
No Harnack chain
Openness Corkscrew condition
Path-connectedness Harnack chain condition
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 5 / 23
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Introduction Main results Strategy of the Proof
Qualitative vs. Quantitative (scale-invariant)
ω σ ω ∈ A∞(σ)
σ(F ) = 0 ⇒ ω(F ) = 0ω(F )
ω(∆).
(σ(F )
σ(∆)
)θ, F ⊂ ∆
Rectifiability Uniform rectifiability
r B∆
crX∆
∂Ω
Ω
No corkscrew
No Harnack chain
Openness Corkscrew condition
Path-connectedness Harnack chain condition
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 5 / 23
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Introduction Main results Strategy of the Proof
Qualitative vs. Quantitative (scale-invariant)
ω σ ω ∈ A∞(σ)
σ(F ) = 0 ⇒ ω(F ) = 0ω(F )
ω(∆).
(σ(F )
σ(∆)
)θ, F ⊂ ∆
Rectifiability Uniform rectifiability
r B∆
crX∆
∂Ω
Ω
No corkscrew
No Harnack chain
Openness Corkscrew condition
Path-connectedness Harnack chain condition
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 5 / 23
![Page 14: Higher integrability of the Harmonic Measure [0.1cm] and ... · PDF fileHigher integrability of the Harmonic Measure and Uniform Recti ability Jos e Mar a Martell joint work with S](https://reader034.vdocuments.us/reader034/viewer/2022051720/5a78b15d7f8b9a852c8e9467/html5/thumbnails/14.jpg)
Introduction Main results Strategy of the Proof
Qualitative vs. Quantitative (scale-invariant)
ω σ ω ∈ A∞(σ)
σ(F ) = 0 ⇒ ω(F ) = 0ω(F )
ω(∆).
(σ(F )
σ(∆)
)θ, F ⊂ ∆
Rectifiability Uniform rectifiability
r B∆
crX∆
∂Ω
Ω
No corkscrew
No Harnack chain
Openness Corkscrew condition
Path-connectedness Harnack chain condition
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 5 / 23
![Page 15: Higher integrability of the Harmonic Measure [0.1cm] and ... · PDF fileHigher integrability of the Harmonic Measure and Uniform Recti ability Jos e Mar a Martell joint work with S](https://reader034.vdocuments.us/reader034/viewer/2022051720/5a78b15d7f8b9a852c8e9467/html5/thumbnails/15.jpg)
Introduction Main results Strategy of the Proof
Qualitative vs. Quantitative (scale-invariant)
ω σ ω ∈ A∞(σ)
σ(F ) = 0 ⇒ ω(F ) = 0ω(F )
ω(∆).
(σ(F )
σ(∆)
)θ, F ⊂ ∆
Rectifiability Uniform rectifiability
r B∆
crX∆
∂Ω
Ω
No corkscrew
No Harnack chain
Openness Corkscrew condition
Path-connectedness Harnack chain condition
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 5 / 23
![Page 16: Higher integrability of the Harmonic Measure [0.1cm] and ... · PDF fileHigher integrability of the Harmonic Measure and Uniform Recti ability Jos e Mar a Martell joint work with S](https://reader034.vdocuments.us/reader034/viewer/2022051720/5a78b15d7f8b9a852c8e9467/html5/thumbnails/16.jpg)
Introduction Main results Strategy of the Proof
Qualitative vs. Quantitative (scale-invariant)
ω σ ω ∈ A∞(σ)
σ(F ) = 0 ⇒ ω(F ) = 0ω(F )
ω(∆).
(σ(F )
σ(∆)
)θ, F ⊂ ∆
Rectifiability Uniform rectifiability
r B∆
crX∆
∂Ω
Ω
No corkscrew
No Harnack chain
Openness Corkscrew condition
Path-connectedness Harnack chain condition
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 5 / 23
![Page 17: Higher integrability of the Harmonic Measure [0.1cm] and ... · PDF fileHigher integrability of the Harmonic Measure and Uniform Recti ability Jos e Mar a Martell joint work with S](https://reader034.vdocuments.us/reader034/viewer/2022051720/5a78b15d7f8b9a852c8e9467/html5/thumbnails/17.jpg)
Introduction Main results Strategy of the Proof
Qualitative vs. Quantitative (scale-invariant)
ω σ ω ∈ A∞(σ)
σ(F ) = 0 ⇒ ω(F ) = 0ω(F )
ω(∆).
(σ(F )
σ(∆)
)θ, F ⊂ ∆
Rectifiability Uniform rectifiability
r B∆
crX∆
∂Ω
Ω
No corkscrew
No Harnack chain
Openness Corkscrew condition
Path-connectedness Harnack chain condition
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 5 / 23
![Page 18: Higher integrability of the Harmonic Measure [0.1cm] and ... · PDF fileHigher integrability of the Harmonic Measure and Uniform Recti ability Jos e Mar a Martell joint work with S](https://reader034.vdocuments.us/reader034/viewer/2022051720/5a78b15d7f8b9a852c8e9467/html5/thumbnails/18.jpg)
Introduction Main results Strategy of the Proof
Qualitative vs. Quantitative (scale-invariant)
ω σ ω ∈ A∞(σ)
σ(F ) = 0 ⇒ ω(F ) = 0ω(F )
ω(∆).
(σ(F )
σ(∆)
)θ, F ⊂ ∆
Rectifiability Uniform rectifiability
r B∆
crX∆
∂Ω
Ω
No corkscrew
No Harnack chain
Openness Corkscrew condition
Path-connectedness Harnack chain condition
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 5 / 23
![Page 19: Higher integrability of the Harmonic Measure [0.1cm] and ... · PDF fileHigher integrability of the Harmonic Measure and Uniform Recti ability Jos e Mar a Martell joint work with S](https://reader034.vdocuments.us/reader034/viewer/2022051720/5a78b15d7f8b9a852c8e9467/html5/thumbnails/19.jpg)
Introduction Main results Strategy of the Proof
Qualitative vs. Quantitative (scale-invariant)
ω σ ω ∈ A∞(σ)
σ(F ) = 0 ⇒ ω(F ) = 0ω(F )
ω(∆).
(σ(F )
σ(∆)
)θ, F ⊂ ∆
Rectifiability Uniform rectifiability
r B∆
crX∆
∂Ω
Ω
No corkscrew
No Harnack chain
Openness Corkscrew condition
Path-connectedness Harnack chain condition
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 5 / 23
![Page 20: Higher integrability of the Harmonic Measure [0.1cm] and ... · PDF fileHigher integrability of the Harmonic Measure and Uniform Recti ability Jos e Mar a Martell joint work with S](https://reader034.vdocuments.us/reader034/viewer/2022051720/5a78b15d7f8b9a852c8e9467/html5/thumbnails/20.jpg)
Introduction Main results Strategy of the Proof
NTA domains
Definition (Jerison-Kenig 1982)
Ω ⊂ Rn+1 is NTA if
Ω satisfies the Corkscrew condition
Ωext = Rn+1 \ Ω satisfies the Corkscrew condition
Ω satisfies the Harnack chain condition
Theorem (David-Jerison 1990; Semmes 1989)
Ω ⊂ Rn+1 is NTA
∂Ω is ADR rn ≈ σ(∆(x, r)), x ∈ ∂Ω
Then ω ∈ A∞(σ).
Corkscrew for Ωext can be relaxed: n-dim. disk in place of a ball
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 6 / 23
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Introduction Main results Strategy of the Proof
NTA domains
Definition (Jerison-Kenig 1982)
Ω ⊂ Rn+1 is NTA if
Ω satisfies the Corkscrew condition
Ωext = Rn+1 \ Ω satisfies the Corkscrew condition
Ω satisfies the Harnack chain condition
Theorem (David-Jerison 1990; Semmes 1989)
Ω ⊂ Rn+1 is NTA
∂Ω is ADR rn ≈ σ(∆(x, r)), x ∈ ∂Ω
Then ω ∈ A∞(σ).
Corkscrew for Ωext can be relaxed: n-dim. disk in place of a ball
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 6 / 23
![Page 22: Higher integrability of the Harmonic Measure [0.1cm] and ... · PDF fileHigher integrability of the Harmonic Measure and Uniform Recti ability Jos e Mar a Martell joint work with S](https://reader034.vdocuments.us/reader034/viewer/2022051720/5a78b15d7f8b9a852c8e9467/html5/thumbnails/22.jpg)
Introduction Main results Strategy of the Proof
NTA domains
Definition (Jerison-Kenig 1982)
Ω ⊂ Rn+1 is NTA if
Ω satisfies the Corkscrew condition
Ωext = Rn+1 \ Ω satisfies the Corkscrew condition
Ω satisfies the Harnack chain condition
Theorem (David-Jerison 1990; Semmes 1989)
Ω ⊂ Rn+1 is NTA
∂Ω is ADR rn ≈ σ(∆(x, r)), x ∈ ∂Ω
Then ω ∈ A∞(σ).
Corkscrew for Ωext can be relaxed: n-dim. disk in place of a ball
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 6 / 23
![Page 23: Higher integrability of the Harmonic Measure [0.1cm] and ... · PDF fileHigher integrability of the Harmonic Measure and Uniform Recti ability Jos e Mar a Martell joint work with S](https://reader034.vdocuments.us/reader034/viewer/2022051720/5a78b15d7f8b9a852c8e9467/html5/thumbnails/23.jpg)
Introduction Main results Strategy of the Proof
NTA domains: Key steps in [David-Jerison 1990]
1 BPBLSD: Big Pieces of Boundaries of Lipschitz Sub-Domains
For every B(x, r), x ∈ ∂Ω,
∃Ω′ ⊂ Ω Lipschitz
“Ample contact”
σ(∂Ω′ ∩ ∂Ω ∩B(x, r)) & rn
Ω
Ω′
2 Maximum principle + [Dahlberg 77]: 0 < η 1 (“Big pieces”)
F ⊂ ∆, σ(F ) ≥ (1− η)σ(∆) =⇒ ωX∆(F ) ≥ c0 > 0 (?)
3 Exterior corkscrew + Harnack chain Comparison principle
(?) self-improves to ω ∈ A∞(σ)
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 7 / 23
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Introduction Main results Strategy of the Proof
NTA domains: Key steps in [David-Jerison 1990]
1 BPBLSD: Big Pieces of Boundaries of Lipschitz Sub-Domains
For every B(x, r), x ∈ ∂Ω,
∃Ω′ ⊂ Ω Lipschitz
“Ample contact”
σ(∂Ω′ ∩ ∂Ω ∩B(x, r)) & rn
Ω
Ω′
2 Maximum principle + [Dahlberg 77]: 0 < η 1 (“Big pieces”)
F ⊂ ∆, σ(F ) ≥ (1− η)σ(∆) =⇒ ωX∆(F ) ≥ c0 > 0 (?)
3 Exterior corkscrew + Harnack chain Comparison principle
(?) self-improves to ω ∈ A∞(σ)
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 7 / 23
![Page 25: Higher integrability of the Harmonic Measure [0.1cm] and ... · PDF fileHigher integrability of the Harmonic Measure and Uniform Recti ability Jos e Mar a Martell joint work with S](https://reader034.vdocuments.us/reader034/viewer/2022051720/5a78b15d7f8b9a852c8e9467/html5/thumbnails/25.jpg)
Introduction Main results Strategy of the Proof
NTA domains: Key steps in [David-Jerison 1990]
1 BPBLSD: Big Pieces of Boundaries of Lipschitz Sub-Domains
For every B(x, r), x ∈ ∂Ω,
∃Ω′ ⊂ Ω Lipschitz
“Ample contact”
σ(∂Ω′ ∩ ∂Ω ∩B(x, r)) & rn
Ω
Ω′
2 Maximum principle + [Dahlberg 77]: 0 < η 1 (“Big pieces”)
F ⊂ ∆, σ(F ) ≥ (1− η)σ(∆) =⇒ ωX∆(F ) ≥ c0 > 0 (?)
3 Exterior corkscrew + Harnack chain Comparison principle
(?) self-improves to ω ∈ A∞(σ)
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 7 / 23
![Page 26: Higher integrability of the Harmonic Measure [0.1cm] and ... · PDF fileHigher integrability of the Harmonic Measure and Uniform Recti ability Jos e Mar a Martell joint work with S](https://reader034.vdocuments.us/reader034/viewer/2022051720/5a78b15d7f8b9a852c8e9467/html5/thumbnails/26.jpg)
Introduction Main results Strategy of the Proof
NTA domains: Key steps in [David-Jerison 1990]
1 BPBLSD: Big Pieces of Boundaries of Lipschitz Sub-Domains
For every B(x, r), x ∈ ∂Ω,
∃Ω′ ⊂ Ω Lipschitz
“Ample contact”
σ(∂Ω′ ∩ ∂Ω ∩B(x, r)) & rn
Ω
Ω′
2 Maximum principle + [Dahlberg 77]: 0 < η 1 (“Big pieces”)
F ⊂ ∆, σ(F ) ≥ (1− η)σ(∆) =⇒ ωX∆(F ) ≥ c0 > 0 (?)
3 Exterior corkscrew + Harnack chain Comparison principle
(?) self-improves to ω ∈ A∞(σ)
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 7 / 23
![Page 27: Higher integrability of the Harmonic Measure [0.1cm] and ... · PDF fileHigher integrability of the Harmonic Measure and Uniform Recti ability Jos e Mar a Martell joint work with S](https://reader034.vdocuments.us/reader034/viewer/2022051720/5a78b15d7f8b9a852c8e9467/html5/thumbnails/27.jpg)
Introduction Main results Strategy of the Proof
NTA domains: Key steps in [David-Jerison 1990]
1 BPBLSD: Big Pieces of Boundaries of Lipschitz Sub-Domains
For every B(x, r), x ∈ ∂Ω,
∃Ω′ ⊂ Ω Lipschitz
“Ample contact”
σ(∂Ω′ ∩ ∂Ω ∩B(x, r)) & rn
Ω
Ω′
2 Maximum principle + [Dahlberg 77]: 0 < η 1 (“Big pieces”)
F ⊂ ∆, σ(F ) ≥ (1− η)σ(∆) =⇒ ωX∆(F ) ≥ c0 > 0 (?)
3 Exterior corkscrew + Harnack chain Comparison principle
(?) self-improves to ω ∈ A∞(σ)
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 7 / 23
![Page 28: Higher integrability of the Harmonic Measure [0.1cm] and ... · PDF fileHigher integrability of the Harmonic Measure and Uniform Recti ability Jos e Mar a Martell joint work with S](https://reader034.vdocuments.us/reader034/viewer/2022051720/5a78b15d7f8b9a852c8e9467/html5/thumbnails/28.jpg)
Introduction Main results Strategy of the Proof
NTA domains: Key steps in [David-Jerison 1990]
1 BPBLSD: Big Pieces of Boundaries of Lipschitz Sub-Domains
For every B(x, r), x ∈ ∂Ω,
∃Ω′ ⊂ Ω Lipschitz
“Ample contact”
σ(∂Ω′ ∩ ∂Ω ∩B(x, r)) & rn
Ω
Ω′
2 Maximum principle + [Dahlberg 77]: 0 < η 1 (“Big pieces”)
F ⊂ ∆, σ(F ) ≥ (1− η)σ(∆) =⇒ ωX∆(F ) ≥ c0 > 0 (?)
3 Exterior corkscrew + Harnack chain Comparison principle
(?) self-improves to ω ∈ A∞(σ)
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 7 / 23
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Introduction Main results Strategy of the Proof
Related results
[Bennewitz-Lewis 2004] Remove ext. corkscrew and Harnack chain
∂Ω ADR Ω interior corkscrew BPBLSD
Maximum principle + [Dahlberg 77]: 0 < η 1
F ⊂ ∆, σ(F ) ≥ (1− η)σ(∆) =⇒ ωX∆(F ) ≥ c0 > 0 (?)
(?) self-improves to “weak-A∞” (“weak Reverse Holder”)(even without comparison principle)
ω(F ) .
(σ(F )
σ(∆)
)θω(2 ∆)
Sharp by counterexample
[Badger 2011] Ω NTA ∂Ω lower ADR: rn . σ(∆(x, r))
BPBLSDJ.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 8 / 23
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Introduction Main results Strategy of the Proof
Related results
[Bennewitz-Lewis 2004] Remove ext. corkscrew and Harnack chain
∂Ω ADR Ω interior corkscrew BPBLSD
Maximum principle + [Dahlberg 77]: 0 < η 1
F ⊂ ∆, σ(F ) ≥ (1− η)σ(∆) =⇒ ωX∆(F ) ≥ c0 > 0 (?)
(?) self-improves to “weak-A∞” (“weak Reverse Holder”)(even without comparison principle)
ω(F ) .
(σ(F )
σ(∆)
)θω(2 ∆)
Sharp by counterexample
[Badger 2011] Ω NTA ∂Ω lower ADR: rn . σ(∆(x, r))
BPBLSDJ.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 8 / 23
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Introduction Main results Strategy of the Proof
Related results
[Bennewitz-Lewis 2004] Remove ext. corkscrew and Harnack chain
∂Ω ADR Ω interior corkscrew BPBLSD
Maximum principle + [Dahlberg 77]: 0 < η 1
F ⊂ ∆, σ(F ) ≥ (1− η)σ(∆) =⇒ ωX∆(F ) ≥ c0 > 0 (?)
(?) self-improves to “weak-A∞” (“weak Reverse Holder”)(even without comparison principle)
ω(F ) .
(σ(F )
σ(∆)
)θω(2 ∆)
Sharp by counterexample
[Badger 2011] Ω NTA ∂Ω lower ADR: rn . σ(∆(x, r))
BPBLSDJ.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 8 / 23
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Introduction Main results Strategy of the Proof
Related results
[Bennewitz-Lewis 2004] Remove ext. corkscrew and Harnack chain
∂Ω ADR Ω interior corkscrew BPBLSD
Maximum principle + [Dahlberg 77]: 0 < η 1
F ⊂ ∆, σ(F ) ≥ (1− η)σ(∆) =⇒ ωX∆(F ) ≥ c0 > 0 (?)
(?) self-improves to “weak-A∞” (“weak Reverse Holder”)(even without comparison principle)
ω(F ) .
(σ(F )
σ(∆)
)θω(2 ∆)
Sharp by counterexample
[Badger 2011] Ω NTA ∂Ω lower ADR: rn . σ(∆(x, r))
BPBLSDJ.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 8 / 23
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Introduction Main results Strategy of the Proof
Related results
[Bennewitz-Lewis 2004] Remove ext. corkscrew and Harnack chain
∂Ω ADR Ω interior corkscrew BPBLSD
Maximum principle + [Dahlberg 77]: 0 < η 1
F ⊂ ∆, σ(F ) ≥ (1− η)σ(∆) =⇒ ωX∆(F ) ≥ c0 > 0 (?)
(?) self-improves to “weak-A∞” (“weak Reverse Holder”)(even without comparison principle)
ω(F ) .
(σ(F )
σ(∆)
)θω(2 ∆)
Sharp by counterexample
[Badger 2011] Ω NTA ∂Ω lower ADR: rn . σ(∆(x, r))
BPBLSDJ.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 8 / 23
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Introduction Main results Strategy of the Proof
Related results
[Bennewitz-Lewis 2004] Remove ext. corkscrew and Harnack chain
∂Ω ADR Ω interior corkscrew BPBLSD
Maximum principle + [Dahlberg 77]: 0 < η 1
F ⊂ ∆, σ(F ) ≥ (1− η)σ(∆) =⇒ ωX∆(F ) ≥ c0 > 0 (?)
(?) self-improves to “weak-A∞” (“weak Reverse Holder”)(even without comparison principle)
ω(F ) .
(σ(F )
σ(∆)
)θω(2 ∆)
Sharp by counterexample
[Badger 2011] Ω NTA ∂Ω lower ADR: rn . σ(∆(x, r))
BPBLSDJ.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 8 / 23
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Introduction Main results Strategy of the Proof
Related results
[Bennewitz-Lewis 2004] Remove ext. corkscrew and Harnack chain
∂Ω ADR Ω interior corkscrew BPBLSD
Maximum principle + [Dahlberg 77]: 0 < η 1
F ⊂ ∆, σ(F ) ≥ (1− η)σ(∆) =⇒ ωX∆(F ) ≥ c0 > 0 (?)
(?) self-improves to “weak-A∞” (“weak Reverse Holder”)(even without comparison principle)
ω(F ) .
(σ(F )
σ(∆)
)θω(2 ∆)
Sharp by counterexample
[Badger 2011] Ω NTA ∂Ω lower ADR: rn . σ(∆(x, r))
BPBLSDJ.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 8 / 23
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Introduction Main results Strategy of the Proof
Uniform rectifiability
Definition
E ⊂ Rn+1 closed ADR is UR if∫Rn+1\E
|∇2Sf(X)|2 dist(X,E) dX ≤ C∫E|f(y)|2 dHn(y)
where Sf single layer potential
Sf(X) := cn
∫E
f(y)
|X − y|n−1dHn(y), X /∈ E
[David-Semmes 1991]
E is UR ⇐⇒ E is ADR + all “nice” SIO are bounded on L2(E)
[Hrycak] UR 6=⇒ Big Pieces of Lipschitz Graphs
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 9 / 23
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Introduction Main results Strategy of the Proof
Uniform rectifiability
Definition
E ⊂ Rn+1 closed ADR is UR if∫Rn+1\E
|∇2Sf(X)|2 dist(X,E) dX ≤ C∫E|f(y)|2 dHn(y)
where Sf single layer potential
Sf(X) := cn
∫E
f(y)
|X − y|n−1dHn(y), X /∈ E
[David-Semmes 1991]
E is UR ⇐⇒ E is ADR + all “nice” SIO are bounded on L2(E)
[Hrycak] UR 6=⇒ Big Pieces of Lipschitz Graphs
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 9 / 23
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Introduction Main results Strategy of the Proof
Uniform rectifiability
Definition
E ⊂ Rn+1 closed ADR is UR if∫Rn+1\E
|∇2Sf(X)|2 dist(X,E) dX ≤ C∫E|f(y)|2 dHn(y)
where Sf single layer potential
Sf(X) := cn
∫E
f(y)
|X − y|n−1dHn(y), X /∈ E
[David-Semmes 1991]
E is UR ⇐⇒ E is ADR + all “nice” SIO are bounded on L2(E)
[Hrycak] UR 6=⇒ Big Pieces of Lipschitz Graphs
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 9 / 23
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Introduction Main results Strategy of the Proof
Qualitative vs. Quantitative (scale-invariant)
Rectifiability Uniform Rectifiablity
Existence approx. tangent planes P. Jones’s β-functionals
β2(x, t) = infP
(1
tn
∫B(x,t)∩E
(dist(y, P )
t
)2
dHn(y)
)1/2
, x ∈ E, t > 0
[David-Semmes 1991] E ADR is UR if and only if
β2(x, t)2 dHn(x)dt
tis a Carleson measure on E × Rn+1
E ADR is UR if and only if
|∇2S1(X)|2 dist(X,E) dX is a Carleson measure on E × Rn+1
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 10 / 23
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Introduction Main results Strategy of the Proof
Qualitative vs. Quantitative (scale-invariant)
Rectifiability Uniform Rectifiablity
Existence approx. tangent planes P. Jones’s β-functionals
β2(x, t) = infP
(1
tn
∫B(x,t)∩E
(dist(y, P )
t
)2
dHn(y)
)1/2
, x ∈ E, t > 0
[David-Semmes 1991] E ADR is UR if and only if
β2(x, t)2 dHn(x)dt
tis a Carleson measure on E × Rn+1
E ADR is UR if and only if
|∇2S1(X)|2 dist(X,E) dX is a Carleson measure on E × Rn+1
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 10 / 23
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Introduction Main results Strategy of the Proof
Qualitative vs. Quantitative (scale-invariant)
Rectifiability Uniform Rectifiablity
Existence approx. tangent planes P. Jones’s β-functionals
β2(x, t) = infP
(1
tn
∫B(x,t)∩E
(dist(y, P )
t
)2
dHn(y)
)1/2
, x ∈ E, t > 0
[David-Semmes 1991] E ADR is UR if and only if
β2(x, t)2 dHn(x)dt
tis a Carleson measure on E × Rn+1
E ADR is UR if and only if
|∇2S1(X)|2 dist(X,E) dX is a Carleson measure on E × Rn+1
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 10 / 23
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Introduction Main results Strategy of the Proof
Qualitative vs. Quantitative (scale-invariant)
Rectifiability Uniform Rectifiablity
Existence approx. tangent planes P. Jones’s β-functionals
β2(x, t) = infP
(1
tn
∫B(x,t)∩E
(dist(y, P )
t
)2
dHn(y)
)1/2
, x ∈ E, t > 0
[David-Semmes 1991] E ADR is UR if and only if
β2(x, t)2 dHn(x)dt
tis a Carleson measure on E × Rn+1
E ADR is UR if and only if
|∇2S1(X)|2 dist(X,E) dX is a Carleson measure on E × Rn+1
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 10 / 23
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Introduction Main results Strategy of the Proof
Qualitative vs. Quantitative (scale-invariant)
Rectifiability Uniform Rectifiablity
Existence approx. tangent planes P. Jones’s β-functionals
β2(x, t) = infP
(1
tn
∫B(x,t)∩E
(dist(y, P )
t
)2
dHn(y)
)1/2
, x ∈ E, t > 0
[David-Semmes 1991] E ADR is UR if and only if
β2(x, t)2 dHn(x)dt
tis a Carleson measure on E × Rn+1
E ADR is UR if and only if
|∇2S1(X)|2 dist(X,E) dX is a Carleson measure on E × Rn+1
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 10 / 23
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Introduction Main results Strategy of the Proof
Section 2
Main results
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 11 / 23
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Introduction Main results Strategy of the Proof
Main results
Theorem
∂Ω ADR Ω interior Corkscrew and Harnack chain
[Hofmann, M.] ∂Ω UR =⇒ ω ∈ Aweak∞ (weak-Reverse Holder)∫
∆(kX∆)q dσ . σ(∆)1−q (RHweak
q )
[Hofmann, Uriarte-Tuero, M.] (RHweakq ) =⇒ ∂Ω UR
No exterior assumptions. No assumption BPBLSD.
ADR + interior Corkscrew + Harnack chain:
∂Ω UR ⇐⇒ ω ∈ Aweak∞ ⇐⇒ ω σ & k ∈ RHweak
q
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 12 / 23
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Introduction Main results Strategy of the Proof
Main results
Theorem
∂Ω ADR Ω interior Corkscrew and Harnack chain
[Hofmann, M.] ∂Ω UR =⇒ ω ∈ Aweak∞ (weak-Reverse Holder)∫
∆(kX∆)q dσ . σ(∆)1−q (RHweak
q )
[Hofmann, Uriarte-Tuero, M.] (RHweakq ) =⇒ ∂Ω UR
No exterior assumptions. No assumption BPBLSD.
ADR + interior Corkscrew + Harnack chain:
∂Ω UR ⇐⇒ ω ∈ Aweak∞ ⇐⇒ ω σ & k ∈ RHweak
q
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 12 / 23
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Introduction Main results Strategy of the Proof
Main results
Theorem
∂Ω ADR Ω interior Corkscrew and Harnack chain
[Hofmann, M.] ∂Ω UR =⇒ ω ∈ Aweak∞ (weak-Reverse Holder)∫
∆(kX∆)q dσ . σ(∆)1−q (RHweak
q )
[Hofmann, Uriarte-Tuero, M.] (RHweakq ) =⇒ ∂Ω UR
No exterior assumptions. No assumption BPBLSD.
ADR + interior Corkscrew + Harnack chain:
∂Ω UR ⇐⇒ ω ∈ Aweak∞ ⇐⇒ ω σ & k ∈ RHweak
q
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 12 / 23
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Introduction Main results Strategy of the Proof
Main results
Theorem
∂Ω ADR Ω interior Corkscrew and Harnack chain
[Hofmann, M.] ∂Ω UR =⇒ ω ∈ Aweak∞ (weak-Reverse Holder)∫
∆(kX∆)q dσ . σ(∆)1−q (RHweak
q )
[Hofmann, Uriarte-Tuero, M.] (RHweakq ) =⇒ ∂Ω UR
No exterior assumptions. No assumption BPBLSD.
ADR + interior Corkscrew + Harnack chain:
∂Ω UR ⇐⇒ ω ∈ Aweak∞ ⇐⇒ ω σ & k ∈ RHweak
q
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 12 / 23
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Introduction Main results Strategy of the Proof
Main results
Theorem
∂Ω ADR Ω interior Corkscrew and Harnack chain
[Hofmann, M.] ∂Ω UR =⇒ ω ∈ Aweak∞ (weak-Reverse Holder)∫
∆(kX∆)q dσ . σ(∆)1−q (RHweak
q )
[Hofmann, Uriarte-Tuero, M.] (RHweakq ) =⇒ ∂Ω UR
No exterior assumptions. No assumption BPBLSD.
ADR + interior Corkscrew + Harnack chain:
∂Ω UR ⇐⇒ ω ∈ Aweak∞ ⇐⇒ ω σ & k ∈ RHweak
q
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 12 / 23
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Introduction Main results Strategy of the Proof
Main results
Theorem
∂Ω ADR Ω interior Corkscrew and Harnack chain
[Hofmann, M.] ∂Ω UR =⇒ ω ∈ Aweak∞ (weak-Reverse Holder)∫
∆(kX∆)q dσ . σ(∆)1−q (RHweak
q )
[Hofmann, Uriarte-Tuero, M.] (RHweakq ) =⇒ ∂Ω UR
No exterior assumptions. No assumption BPBLSD.
ADR + interior Corkscrew + Harnack chain:
∂Ω UR ⇐⇒ ω ∈ Aweak∞ ⇐⇒ ω σ & k ∈ RHweak
q
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 12 / 23
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Introduction Main results Strategy of the Proof
“Large constant” analogue of Kenig-Toro 1997-2003
[Kenig-Toro] ∂Ω ADR Reifenberg flatness
Ω “vanishing chord-arc” ⇐⇒ log k ∈ VMO
[Hofmann-Lewis-Nystrom] + [Hofmann-Mitrea-Taylor]
“vanishing chord-arc” ⇐⇒ 2-sided NTA + “Vanishing UR”
[Kenig-Toro] “Vanishing UR” ⇐⇒ log k ∈ VMO
[Hofmann, M], [Hofmann, Uriarte-Tuero, M.]
UR “⇐⇒” ω ∈ A∞ “⇐⇒” log k ∈ BMO
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 13 / 23
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Introduction Main results Strategy of the Proof
“Large constant” analogue of Kenig-Toro 1997-2003
[Kenig-Toro] ∂Ω ADR Reifenberg flatness
Ω “vanishing chord-arc” ⇐⇒ log k ∈ VMO
[Hofmann-Lewis-Nystrom] + [Hofmann-Mitrea-Taylor]
“vanishing chord-arc” ⇐⇒ 2-sided NTA + “Vanishing UR”
[Kenig-Toro] “Vanishing UR” ⇐⇒ log k ∈ VMO
[Hofmann, M], [Hofmann, Uriarte-Tuero, M.]
UR “⇐⇒” ω ∈ A∞ “⇐⇒” log k ∈ BMO
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 13 / 23
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Introduction Main results Strategy of the Proof
“Large constant” analogue of Kenig-Toro 1997-2003
[Kenig-Toro] ∂Ω ADR Reifenberg flatness
Ω “vanishing chord-arc” ⇐⇒ log k ∈ VMO
[Hofmann-Lewis-Nystrom] + [Hofmann-Mitrea-Taylor]
“vanishing chord-arc” ⇐⇒ 2-sided NTA + “Vanishing UR”
[Kenig-Toro] “Vanishing UR” ⇐⇒ log k ∈ VMO
[Hofmann, M], [Hofmann, Uriarte-Tuero, M.]
UR “⇐⇒” ω ∈ A∞ “⇐⇒” log k ∈ BMO
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 13 / 23
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Introduction Main results Strategy of the Proof
“Large constant” analogue of Kenig-Toro 1997-2003
[Kenig-Toro] ∂Ω ADR Reifenberg flatness
Ω “vanishing chord-arc” ⇐⇒ log k ∈ VMO
[Hofmann-Lewis-Nystrom] + [Hofmann-Mitrea-Taylor]
“vanishing chord-arc” ⇐⇒ 2-sided NTA + “Vanishing UR”
[Kenig-Toro] “Vanishing UR” ⇐⇒ log k ∈ VMO
[Hofmann, M], [Hofmann, Uriarte-Tuero, M.]
UR “⇐⇒” ω ∈ A∞ “⇐⇒” log k ∈ BMO
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 13 / 23
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Introduction Main results Strategy of the Proof
Section 3
Strategy of the Proof
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 14 / 23
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Introduction Main results Strategy of the Proof
Strategy of the Proof: w ∈ Aweak∞ (σ) =⇒ UR
Hypotheses
∂Ω ADR Ω interior Corkscrew and Harnack chain∫∆
(kX∆)q dσ . σ(∆)1−q (RHweakq )
1 Approximating domains: ΩN
(RHweakq ) passes uniformly to ΩN
2 UR for approximating domains ΩN (uniformly in N)
Local Tb theorem for square functions
3 UR for Ω
All “nice” SIO are bounded on are bounded on L2(∂Ω)
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 15 / 23
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Introduction Main results Strategy of the Proof
Strategy of the Proof: w ∈ Aweak∞ (σ) =⇒ UR
Hypotheses
∂Ω ADR Ω interior Corkscrew and Harnack chain∫∆
(kX∆)q dσ . σ(∆)1−q (RHweakq )
1 Approximating domains: ΩN
(RHweakq ) passes uniformly to ΩN
2 UR for approximating domains ΩN (uniformly in N)
Local Tb theorem for square functions
3 UR for Ω
All “nice” SIO are bounded on are bounded on L2(∂Ω)
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 15 / 23
![Page 58: Higher integrability of the Harmonic Measure [0.1cm] and ... · PDF fileHigher integrability of the Harmonic Measure and Uniform Recti ability Jos e Mar a Martell joint work with S](https://reader034.vdocuments.us/reader034/viewer/2022051720/5a78b15d7f8b9a852c8e9467/html5/thumbnails/58.jpg)
Introduction Main results Strategy of the Proof
Strategy of the Proof: w ∈ Aweak∞ (σ) =⇒ UR
Hypotheses
∂Ω ADR Ω interior Corkscrew and Harnack chain∫∆
(kX∆)q dσ . σ(∆)1−q (RHweakq )
1 Approximating domains: ΩN
(RHweakq ) passes uniformly to ΩN
2 UR for approximating domains ΩN (uniformly in N)
Local Tb theorem for square functions
3 UR for Ω
All “nice” SIO are bounded on are bounded on L2(∂Ω)
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 15 / 23
![Page 59: Higher integrability of the Harmonic Measure [0.1cm] and ... · PDF fileHigher integrability of the Harmonic Measure and Uniform Recti ability Jos e Mar a Martell joint work with S](https://reader034.vdocuments.us/reader034/viewer/2022051720/5a78b15d7f8b9a852c8e9467/html5/thumbnails/59.jpg)
Introduction Main results Strategy of the Proof
Strategy of the Proof: w ∈ Aweak∞ (σ) =⇒ UR
Hypotheses
∂Ω ADR Ω interior Corkscrew and Harnack chain∫∆
(kX∆)q dσ . σ(∆)1−q (RHweakq )
1 Approximating domains: ΩN
(RHweakq ) passes uniformly to ΩN
2 UR for approximating domains ΩN (uniformly in N)
Local Tb theorem for square functions
3 UR for Ω
All “nice” SIO are bounded on are bounded on L2(∂Ω)
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 15 / 23
![Page 60: Higher integrability of the Harmonic Measure [0.1cm] and ... · PDF fileHigher integrability of the Harmonic Measure and Uniform Recti ability Jos e Mar a Martell joint work with S](https://reader034.vdocuments.us/reader034/viewer/2022051720/5a78b15d7f8b9a852c8e9467/html5/thumbnails/60.jpg)
Introduction Main results Strategy of the Proof
Strategy of the Proof: w ∈ Aweak∞ (σ) =⇒ UR
1 Approximating domains
ΩN Ω approximating domains
ΩN inherits ADR, Int. corkscrew, Harnack chain uniformly
∂ΩN “faces” of Whitney cubes of size approx. 2−N
ΩN satisfies “qualitative assumptions”:
Wiener test holds at all boundary points
CFMS(Caffarelli-Fabes-Mortola-Salsa) holds qualitatively
1
CN
ωXN (∆N )
σN (∆N )≤ GN (X∆N
, X)
δN (X∆N)≤ C
ωXN (∆N )
σN (∆N ), X ∈ ΩN \ 2B
Not always true
Always holds by Harnack Chain
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 16 / 23
![Page 61: Higher integrability of the Harmonic Measure [0.1cm] and ... · PDF fileHigher integrability of the Harmonic Measure and Uniform Recti ability Jos e Mar a Martell joint work with S](https://reader034.vdocuments.us/reader034/viewer/2022051720/5a78b15d7f8b9a852c8e9467/html5/thumbnails/61.jpg)
Introduction Main results Strategy of the Proof
Strategy of the Proof: w ∈ Aweak∞ (σ) =⇒ UR
1 Approximating domains
ΩN Ω approximating domains
ΩN inherits ADR, Int. corkscrew, Harnack chain uniformly
∂ΩN “faces” of Whitney cubes of size approx. 2−N
ΩN satisfies “qualitative assumptions”:
Wiener test holds at all boundary points
CFMS(Caffarelli-Fabes-Mortola-Salsa) holds qualitatively
1
CN
ωXN (∆N )
σN (∆N )≤ GN (X∆N
, X)
δN (X∆N)≤ C
ωXN (∆N )
σN (∆N ), X ∈ ΩN \ 2B
Not always true
Always holds by Harnack Chain
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 16 / 23
![Page 62: Higher integrability of the Harmonic Measure [0.1cm] and ... · PDF fileHigher integrability of the Harmonic Measure and Uniform Recti ability Jos e Mar a Martell joint work with S](https://reader034.vdocuments.us/reader034/viewer/2022051720/5a78b15d7f8b9a852c8e9467/html5/thumbnails/62.jpg)
Introduction Main results Strategy of the Proof
Strategy of the Proof: w ∈ Aweak∞ (σ) =⇒ UR
1 Approximating domains
ΩN Ω approximating domains
ΩN inherits ADR, Int. corkscrew, Harnack chain uniformly
∂ΩN “faces” of Whitney cubes of size approx. 2−N
ΩN satisfies “qualitative assumptions”:
Wiener test holds at all boundary points
CFMS(Caffarelli-Fabes-Mortola-Salsa) holds qualitatively
1
CN
ωXN (∆N )
σN (∆N )≤ GN (X∆N
, X)
δN (X∆N)≤ C
ωXN (∆N )
σN (∆N ), X ∈ ΩN \ 2B
Not always true
Always holds by Harnack Chain
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 16 / 23
![Page 63: Higher integrability of the Harmonic Measure [0.1cm] and ... · PDF fileHigher integrability of the Harmonic Measure and Uniform Recti ability Jos e Mar a Martell joint work with S](https://reader034.vdocuments.us/reader034/viewer/2022051720/5a78b15d7f8b9a852c8e9467/html5/thumbnails/63.jpg)
Introduction Main results Strategy of the Proof
Strategy of the Proof: w ∈ Aweak∞ (σ) =⇒ UR
1 Approximating domains
ΩN Ω approximating domains
ΩN inherits ADR, Int. corkscrew, Harnack chain uniformly
∂ΩN “faces” of Whitney cubes of size approx. 2−N
ΩN satisfies “qualitative assumptions”:
Wiener test holds at all boundary points
CFMS(Caffarelli-Fabes-Mortola-Salsa) holds qualitatively
1
CN
ωXN (∆N )
σN (∆N )≤ GN (X∆N
, X)
δN (X∆N)≤ C
ωXN (∆N )
σN (∆N ), X ∈ ΩN \ 2B
Not always true
Always holds by Harnack Chain
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 16 / 23
![Page 64: Higher integrability of the Harmonic Measure [0.1cm] and ... · PDF fileHigher integrability of the Harmonic Measure and Uniform Recti ability Jos e Mar a Martell joint work with S](https://reader034.vdocuments.us/reader034/viewer/2022051720/5a78b15d7f8b9a852c8e9467/html5/thumbnails/64.jpg)
Introduction Main results Strategy of the Proof
Strategy of the Proof: w ∈ Aweak∞ (σ) =⇒ UR
1 Approximating domains
ΩN Ω approximating domains
ΩN inherits ADR, Int. corkscrew, Harnack chain uniformly
∂ΩN “faces” of Whitney cubes of size approx. 2−N
ΩN satisfies “qualitative assumptions”:
Wiener test holds at all boundary points
CFMS(Caffarelli-Fabes-Mortola-Salsa) holds qualitatively
1
CN
ωXN (∆N )
σN (∆N )≤ GN (X∆N
, X)
δN (X∆N)≤ C
ωXN (∆N )
σN (∆N ), X ∈ ΩN \ 2B
Not always true
Always holds by Harnack Chain
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 16 / 23
![Page 65: Higher integrability of the Harmonic Measure [0.1cm] and ... · PDF fileHigher integrability of the Harmonic Measure and Uniform Recti ability Jos e Mar a Martell joint work with S](https://reader034.vdocuments.us/reader034/viewer/2022051720/5a78b15d7f8b9a852c8e9467/html5/thumbnails/65.jpg)
Introduction Main results Strategy of the Proof
Strategy of the Proof: w ∈ Aweak∞ (σ) =⇒ UR
1 Approximating domains
ΩN Ω approximating domains
ΩN inherits ADR, Int. corkscrew, Harnack chain uniformly
∂ΩN “faces” of Whitney cubes of size approx. 2−N
ΩN satisfies “qualitative assumptions”:
Wiener test holds at all boundary points
CFMS(Caffarelli-Fabes-Mortola-Salsa) holds qualitatively
1
CN
ωXN (∆N )
σN (∆N )≤ GN (X∆N
, X)
δN (X∆N)≤ C
ωXN (∆N )
σN (∆N ), X ∈ ΩN \ 2B
Not always true
Always holds by Harnack Chain
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 16 / 23
![Page 66: Higher integrability of the Harmonic Measure [0.1cm] and ... · PDF fileHigher integrability of the Harmonic Measure and Uniform Recti ability Jos e Mar a Martell joint work with S](https://reader034.vdocuments.us/reader034/viewer/2022051720/5a78b15d7f8b9a852c8e9467/html5/thumbnails/66.jpg)
Introduction Main results Strategy of the Proof
Strategy of the Proof: w ∈ Aweak∞ (σ) =⇒ UR
1 Approximating domains
ΩN Ω approximating domains
ΩN inherits ADR, Int. corkscrew, Harnack chain uniformly
∂ΩN “faces” of Whitney cubes of size approx. 2−N
ΩN satisfies “qualitative assumptions”:
Wiener test holds at all boundary points
CFMS(Caffarelli-Fabes-Mortola-Salsa) holds qualitatively
1
CN
ωXN (∆N )
σN (∆N )≤ GN (X∆N
, X)
δN (X∆N)≤ C
ωXN (∆N )
σN (∆N ), X ∈ ΩN \ 2B
Not always true
Always holds by Harnack Chain
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 16 / 23
![Page 67: Higher integrability of the Harmonic Measure [0.1cm] and ... · PDF fileHigher integrability of the Harmonic Measure and Uniform Recti ability Jos e Mar a Martell joint work with S](https://reader034.vdocuments.us/reader034/viewer/2022051720/5a78b15d7f8b9a852c8e9467/html5/thumbnails/67.jpg)
Introduction Main results Strategy of the Proof
Strategy of the Proof: w ∈ Aweak∞ (σ) =⇒ UR
1 Approximating domains
ΩN Ω approximating domains
ΩN inherits ADR, Int. corkscrew, Harnack chain uniformly
∂ΩN “faces” of Whitney cubes of size approx. 2−N
ΩN satisfies “qualitative assumptions”:
Wiener test holds at all boundary points
CFMS(Caffarelli-Fabes-Mortola-Salsa) holds qualitatively
1
CN
ωXN (∆N )
σN (∆N )≤ GN (X∆N
, X)
δN (X∆N)≤ C
ωXN (∆N )
σN (∆N ), X ∈ ΩN \ 2B
Not always true
Always holds by Harnack Chain
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 16 / 23
![Page 68: Higher integrability of the Harmonic Measure [0.1cm] and ... · PDF fileHigher integrability of the Harmonic Measure and Uniform Recti ability Jos e Mar a Martell joint work with S](https://reader034.vdocuments.us/reader034/viewer/2022051720/5a78b15d7f8b9a852c8e9467/html5/thumbnails/68.jpg)
Introduction Main results Strategy of the Proof
Strategy of the Proof: w ∈ Aweak∞ (σ) =⇒ UR
1 Approximating domains
ΩN Ω approximating domains
ΩN inherits ADR, Int. corkscrew, Harnack chain uniformly
∂ΩN “faces” of Whitney cubes of size approx. 2−N
ΩN satisfies “qualitative assumptions”:
Wiener test holds at all boundary points
CFMS(Caffarelli-Fabes-Mortola-Salsa) holds qualitatively
1
CN
ωXN (∆N )
σN (∆N )≤ GN (X∆N
, X)
δN (X∆N)≤ C
ωXN (∆N )
σN (∆N ), X ∈ ΩN \ 2B
Not always true
Always holds by Harnack Chain
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 16 / 23
![Page 69: Higher integrability of the Harmonic Measure [0.1cm] and ... · PDF fileHigher integrability of the Harmonic Measure and Uniform Recti ability Jos e Mar a Martell joint work with S](https://reader034.vdocuments.us/reader034/viewer/2022051720/5a78b15d7f8b9a852c8e9467/html5/thumbnails/69.jpg)
Introduction Main results Strategy of the Proof
Strategy of the Proof: w ∈ Aweak∞ (σ) =⇒ UR
1 Approximating domains
ΩN Ω approximating domains
ΩN inherits ADR, Int. corkscrew, Harnack chain uniformly
∂ΩN “faces” of Whitney cubes of size approx. 2−N
ΩN satisfies “qualitative assumptions”:
Wiener test holds at all boundary points
CFMS(Caffarelli-Fabes-Mortola-Salsa) holds qualitatively
1
CN
ωXN (∆N )
σN (∆N )≤ GN (X∆N
, X)
δN (X∆N)≤ C
ωXN (∆N )
σN (∆N ), X ∈ ΩN \ 2B
Not always true
Always holds by Harnack Chain
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 16 / 23
![Page 70: Higher integrability of the Harmonic Measure [0.1cm] and ... · PDF fileHigher integrability of the Harmonic Measure and Uniform Recti ability Jos e Mar a Martell joint work with S](https://reader034.vdocuments.us/reader034/viewer/2022051720/5a78b15d7f8b9a852c8e9467/html5/thumbnails/70.jpg)
Introduction Main results Strategy of the Proof
Strategy of the Proof: w ∈ Aweak∞ (σ) =⇒ UR
1 Approximating domains
Proposition (Hofmann, M.)
ΩN satisfies CFMS “quantitatively” (i.e., uniformly in N)
ωXN (∆N )
σN (∆N )≈ GN (X∆N
, X)
δN (X∆N)
, X ∈ ΩN \ 2B
As a consequence,
ωN is doubling (uniformly in N)
Comparison principle holds for GN (uniformly in N)
(RHweakq ) passes uniformly to ΩN (with smaller q)
Reduce to scales . 2−N
Use full comparison principle in some NTA sub-domain(uniformly in N)J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 17 / 23
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Introduction Main results Strategy of the Proof
Strategy of the Proof: w ∈ Aweak∞ (σ) =⇒ UR
1 Approximating domains
Proposition (Hofmann, M.)
ΩN satisfies CFMS “quantitatively” (i.e., uniformly in N)
ωXN (∆N )
σN (∆N )≈ GN (X∆N
, X)
δN (X∆N)
, X ∈ ΩN \ 2B
As a consequence,
ωN is doubling (uniformly in N)
Comparison principle holds for GN (uniformly in N)
(RHweakq ) passes uniformly to ΩN (with smaller q)
Reduce to scales . 2−N
Use full comparison principle in some NTA sub-domain(uniformly in N)J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 17 / 23
![Page 72: Higher integrability of the Harmonic Measure [0.1cm] and ... · PDF fileHigher integrability of the Harmonic Measure and Uniform Recti ability Jos e Mar a Martell joint work with S](https://reader034.vdocuments.us/reader034/viewer/2022051720/5a78b15d7f8b9a852c8e9467/html5/thumbnails/72.jpg)
Introduction Main results Strategy of the Proof
Strategy of the Proof: w ∈ Aweak∞ (σ) =⇒ UR
1 Approximating domains
Proposition (Hofmann, M.)
ΩN satisfies CFMS “quantitatively” (i.e., uniformly in N)
ωXN (∆N )
σN (∆N )≈ GN (X∆N
, X)
δN (X∆N)
, X ∈ ΩN \ 2B
As a consequence,
ωN is doubling (uniformly in N)
Comparison principle holds for GN (uniformly in N)
(RHweakq ) passes uniformly to ΩN (with smaller q)
Reduce to scales . 2−N
Use full comparison principle in some NTA sub-domain(uniformly in N)J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 17 / 23
![Page 73: Higher integrability of the Harmonic Measure [0.1cm] and ... · PDF fileHigher integrability of the Harmonic Measure and Uniform Recti ability Jos e Mar a Martell joint work with S](https://reader034.vdocuments.us/reader034/viewer/2022051720/5a78b15d7f8b9a852c8e9467/html5/thumbnails/73.jpg)
Introduction Main results Strategy of the Proof
Strategy of the Proof: w ∈ Aweak∞ (σ) =⇒ UR
1 Approximating domains
Proposition (Hofmann, M.)
ΩN satisfies CFMS “quantitatively” (i.e., uniformly in N)
ωXN (∆N )
σN (∆N )≈ GN (X∆N
, X)
δN (X∆N)
, X ∈ ΩN \ 2B
As a consequence,
ωN is doubling (uniformly in N)
Comparison principle holds for GN (uniformly in N)
(RHweakq ) passes uniformly to ΩN (with smaller q)
Reduce to scales . 2−N
Use full comparison principle in some NTA sub-domain(uniformly in N)J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 17 / 23
![Page 74: Higher integrability of the Harmonic Measure [0.1cm] and ... · PDF fileHigher integrability of the Harmonic Measure and Uniform Recti ability Jos e Mar a Martell joint work with S](https://reader034.vdocuments.us/reader034/viewer/2022051720/5a78b15d7f8b9a852c8e9467/html5/thumbnails/74.jpg)
Introduction Main results Strategy of the Proof
Strategy of the Proof: w ∈ Aweak∞ (σ) =⇒ UR
2 UR for approximating domains ΩN (uniformly in N)
Ω ≡ ΩN
∂Ω is UR iff
∫∂ΩSf(x)2 dσ(x) ≈
∫Rn+1
|∇2Sf(Y )|2 δ(Y ) dY . ‖f‖L2(∂Ω)
Conical square function Sf(x) =(∫∫
Γ±(x)|∇2Sf(Y )|2 dY
δ(Y )n−1
) 12
Need to show that S is bounded on L2(∂Ω)
Tb theory (Painleve problem: Chirst, Mattila-Melnikov-Verdera,
David, Nazarov-Treil-Volberg, Tolsa)
“Local Tb” for square functions: b bQQ∈D(∂Ω)
(Kato conjecture: Auscher-Hofmann-Lacey-McIntosh-Tchamitchian)J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 18 / 23
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Introduction Main results Strategy of the Proof
Strategy of the Proof: w ∈ Aweak∞ (σ) =⇒ UR
2 UR for approximating domains ΩN (uniformly in N)
Ω ≡ ΩN
∂Ω is UR iff
∫∂ΩSf(x)2 dσ(x) ≈
∫Rn+1
|∇2Sf(Y )|2 δ(Y ) dY . ‖f‖L2(∂Ω)
Conical square function Sf(x) =(∫∫
Γ±(x)|∇2Sf(Y )|2 dY
δ(Y )n−1
) 12
Need to show that S is bounded on L2(∂Ω)
Tb theory (Painleve problem: Chirst, Mattila-Melnikov-Verdera,
David, Nazarov-Treil-Volberg, Tolsa)
“Local Tb” for square functions: b bQQ∈D(∂Ω)
(Kato conjecture: Auscher-Hofmann-Lacey-McIntosh-Tchamitchian)J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 18 / 23
![Page 76: Higher integrability of the Harmonic Measure [0.1cm] and ... · PDF fileHigher integrability of the Harmonic Measure and Uniform Recti ability Jos e Mar a Martell joint work with S](https://reader034.vdocuments.us/reader034/viewer/2022051720/5a78b15d7f8b9a852c8e9467/html5/thumbnails/76.jpg)
Introduction Main results Strategy of the Proof
Strategy of the Proof: w ∈ Aweak∞ (σ) =⇒ UR
2 UR for approximating domains ΩN (uniformly in N)
Ω ≡ ΩN
∂Ω is UR iff
∫∂ΩSf(x)2 dσ(x) ≈
∫Rn+1
|∇2Sf(Y )|2 δ(Y ) dY . ‖f‖L2(∂Ω)
Conical square function Sf(x) =(∫∫
Γ±(x)|∇2Sf(Y )|2 dY
δ(Y )n−1
) 12
Need to show that S is bounded on L2(∂Ω)
Tb theory (Painleve problem: Chirst, Mattila-Melnikov-Verdera,
David, Nazarov-Treil-Volberg, Tolsa)
“Local Tb” for square functions: b bQQ∈D(∂Ω)
(Kato conjecture: Auscher-Hofmann-Lacey-McIntosh-Tchamitchian)J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 18 / 23
![Page 77: Higher integrability of the Harmonic Measure [0.1cm] and ... · PDF fileHigher integrability of the Harmonic Measure and Uniform Recti ability Jos e Mar a Martell joint work with S](https://reader034.vdocuments.us/reader034/viewer/2022051720/5a78b15d7f8b9a852c8e9467/html5/thumbnails/77.jpg)
Introduction Main results Strategy of the Proof
Strategy of the Proof: w ∈ Aweak∞ (σ) =⇒ UR
2 UR for approximating domains ΩN (uniformly in N)
Ω ≡ ΩN
∂Ω is UR iff∫∂ΩSf(x)2 dσ(x) ≈
∫Rn+1
|∇2Sf(Y )|2 δ(Y ) dY . ‖f‖L2(∂Ω)
Conical square function Sf(x) =(∫∫
Γ±(x)|∇2Sf(Y )|2 dY
δ(Y )n−1
) 12
Need to show that S is bounded on L2(∂Ω)
Tb theory (Painleve problem: Chirst, Mattila-Melnikov-Verdera,
David, Nazarov-Treil-Volberg, Tolsa)
“Local Tb” for square functions: b bQQ∈D(∂Ω)
(Kato conjecture: Auscher-Hofmann-Lacey-McIntosh-Tchamitchian)J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 18 / 23
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Introduction Main results Strategy of the Proof
Strategy of the Proof: w ∈ Aweak∞ (σ) =⇒ UR
2 UR for approximating domains ΩN (uniformly in N)
Ω ≡ ΩN
∂Ω is UR iff∫∂ΩSf(x)2 dσ(x) ≈
∫Rn+1
|∇2Sf(Y )|2 δ(Y ) dY . ‖f‖L2(∂Ω)
Conical square function Sf(x) =(∫∫
Γ±(x)|∇2Sf(Y )|2 dY
δ(Y )n−1
) 12
Need to show that S is bounded on L2(∂Ω)
Tb theory (Painleve problem: Chirst, Mattila-Melnikov-Verdera,
David, Nazarov-Treil-Volberg, Tolsa)
“Local Tb” for square functions: b bQQ∈D(∂Ω)
(Kato conjecture: Auscher-Hofmann-Lacey-McIntosh-Tchamitchian)J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 18 / 23
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Introduction Main results Strategy of the Proof
Strategy of the Proof: w ∈ Aweak∞ (σ) =⇒ UR
2 UR for approximating domains ΩN (uniformly in N)
Ω ≡ ΩN
∂Ω is UR iff∫∂ΩSf(x)2 dσ(x) ≈
∫Rn+1
|∇2Sf(Y )|2 δ(Y ) dY . ‖f‖L2(∂Ω)
Conical square function Sf(x) =(∫∫
Γ±(x)|∇2Sf(Y )|2 dY
δ(Y )n−1
) 12
Need to show that S is bounded on L2(∂Ω)
Tb theory (Painleve problem: Chirst, Mattila-Melnikov-Verdera,
David, Nazarov-Treil-Volberg, Tolsa)
“Local Tb” for square functions: b bQQ∈D(∂Ω)
(Kato conjecture: Auscher-Hofmann-Lacey-McIntosh-Tchamitchian)J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 18 / 23
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Introduction Main results Strategy of the Proof
Strategy of the Proof: w ∈ Aweak∞ (σ) =⇒ UR
2 UR for approximating domains ΩN (uniformly in N)
Ω ≡ ΩN
∂Ω is UR iff∫∂ΩSf(x)2 dσ(x) ≈
∫Rn+1
|∇2Sf(Y )|2 δ(Y ) dY . ‖f‖L2(∂Ω)
Conical square function Sf(x) =(∫∫
Γ±(x)|∇2Sf(Y )|2 dY
δ(Y )n−1
) 12
Need to show that S is bounded on L2(∂Ω)
Tb theory (Painleve problem: Chirst, Mattila-Melnikov-Verdera,
David, Nazarov-Treil-Volberg, Tolsa)
“Local Tb” for square functions: b bQQ∈D(∂Ω)
(Kato conjecture: Auscher-Hofmann-Lacey-McIntosh-Tchamitchian)J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 18 / 23
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Introduction Main results Strategy of the Proof
Strategy of the Proof: Local Tb for square functions
Theorem (Grau de la Herran-Mourgoglou)
Ω ⊂ Rn+1 connected and open ∂Ω ADR 1 < q ≤ 2
bQQ∈D(∂Ω) verify
1
∫∂Ω|bQ|q dσ . σ(Q) 2
∣∣∣ ∫QbQ dσ
∣∣∣ & σ(Q)
3
∫Q
(SQbQ)q dσ . σ(Q)
Then S : L2(∂Ω) −→ L2(∂Ω) ∂Ω is UR
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 19 / 23
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Introduction Main results Strategy of the Proof
Strategy of the Proof: Local Tb for square functions
Theorem (Grau de la Herran-Mourgoglou)
Ω ⊂ Rn+1 connected and open ∂Ω ADR 1 < q ≤ 2
bQQ∈D(∂Ω) verify
1
∫∂Ω|bQ|q dσ . σ(Q) 2
∣∣∣ ∫QbQ dσ
∣∣∣ & σ(Q)
3
∫Q
(SQbQ)q dσ . σ(Q)
Then S : L2(∂Ω) −→ L2(∂Ω) ∂Ω is UR
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 19 / 23
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Introduction Main results Strategy of the Proof
Strategy of the Proof: Local Tb for square functions
Theorem (Grau de la Herran-Mourgoglou)
Ω ⊂ Rn+1 connected and open ∂Ω ADR 1 < q ≤ 2
bQQ∈D(∂Ω) verify
1
∫∂Ω|bQ|q dσ . σ(Q) 2
∣∣∣ ∫QbQ dσ
∣∣∣ & σ(Q)
3
∫Q
(SQbQ)q dσ . σ(Q)
Then S : L2(∂Ω) −→ L2(∂Ω) ∂Ω is UR
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 19 / 23
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Introduction Main results Strategy of the Proof
Strategy of the Proof: Local Tb for square functions
Theorem (Grau de la Herran-Mourgoglou)
Ω ⊂ Rn+1 connected and open ∂Ω ADR 1 < q ≤ 2
bQQ∈D(∂Ω) verify
1
∫∂Ω|bQ|q dσ . σ(Q) 2
∣∣∣ ∫QbQ dσ
∣∣∣ & σ(Q)
3
∫Q
(SQbQ)q dσ . σ(Q)
Then S : L2(∂Ω) −→ L2(∂Ω) ∂Ω is UR
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 19 / 23
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Introduction Main results Strategy of the Proof
Strategy of the Proof: Local Tb for square functions
Theorem (Grau de la Herran-Mourgoglou)
Ω ⊂ Rn+1 connected and open ∂Ω ADR 1 < q ≤ 2
bQQ∈D(∂Ω) verify
1
∫∂Ω|bQ|q dσ . σ(Q) 2
∣∣∣ ∫QbQ dσ
∣∣∣ & σ(Q)
3
∫Q
(SQbQ)q dσ . σ(Q)
Then S : L2(∂Ω) −→ L2(∂Ω) ∂Ω is UR
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 19 / 23
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Introduction Main results Strategy of the Proof
Strategy of the Proof: Local Tb for square functions
Theorem (Grau de la Herran-Mourgoglou)
Ω ⊂ Rn+1 connected and open ∂Ω ADR 1 < q ≤ 2
bQQ∈D(∂Ω) verify
1
∫∂Ω|bQ|q dσ . σ(Q) 2
∣∣∣ ∫QbQ dσ
∣∣∣ & σ(Q)
3
∫Q
(SQbQ)q dσ . σ(Q)
Then S : L2(∂Ω) −→ L2(∂Ω) ∂Ω is UR
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 19 / 23
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Introduction Main results Strategy of the Proof
Strategy of the Proof: Local Tb for square functions
Theorem (Grau de la Herran-Mourgoglou)
Ω ⊂ Rn+1 connected and open ∂Ω ADR 1 < q ≤ 2
bQQ∈D(∂Ω) verify
1
∫∂Ω|bQ|q dσ . σ(Q) 2
∣∣∣ ∫QbQ dσ
∣∣∣ & σ(Q)
3
∫Q
(SQbQ)q dσ . σ(Q)
Then S : L2(∂Ω) −→ L2(∂Ω) ∂Ω is UR
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 19 / 23
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Introduction Main results Strategy of the Proof
Strategy of the Proof: Local Tb for square functions
bQ = σ(Q) ηQ kXQ (normalized and localized Poisson kernel)
1
∫∂Ω|bQ|q dσ . σ(Q)q
∫Q
(kXQ)q dσ(RHweak
q )
. σ(Q)
2
∣∣∣ ∫QbQ dσ
∣∣∣ & σ(Q)ωXQ(Q)[Bourgain]
& σ(Q)
3
∫Q
(SQbQ)q dσ . σ(Q)?
SQbQ(x) =(∫∫
Γ±(x)∩BQ
|∇2SbQ(Y )|2 dY
δ(Y )n−1
) 12
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 20 / 23
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Introduction Main results Strategy of the Proof
Strategy of the Proof: Local Tb for square functions
bQ = σ(Q) ηQ kXQ (normalized and localized Poisson kernel)
1
∫∂Ω|bQ|q dσ . σ(Q)q
∫Q
(kXQ)q dσ(RHweak
q )
. σ(Q)
2
∣∣∣ ∫QbQ dσ
∣∣∣ & σ(Q)ωXQ(Q)[Bourgain]
& σ(Q)
3
∫Q
(SQbQ)q dσ . σ(Q)?
SQbQ(x) =(∫∫
Γ±(x)∩BQ
|∇2SbQ(Y )|2 dY
δ(Y )n−1
) 12
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 20 / 23
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Introduction Main results Strategy of the Proof
Strategy of the Proof: Local Tb for square functions
bQ = σ(Q) ηQ kXQ (normalized and localized Poisson kernel)
1
∫∂Ω|bQ|q dσ . σ(Q)q
∫Q
(kXQ)q dσ(RHweak
q )
. σ(Q)
2
∣∣∣ ∫QbQ dσ
∣∣∣ & σ(Q)ωXQ(Q)[Bourgain]
& σ(Q)
3
∫Q
(SQbQ)q dσ . σ(Q)?
SQbQ(x) =(∫∫
Γ±(x)∩BQ
|∇2SbQ(Y )|2 dY
δ(Y )n−1
) 12
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 20 / 23
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Introduction Main results Strategy of the Proof
Strategy of the Proof: Local Tb for square functions
bQ = σ(Q) ηQ kXQ (normalized and localized Poisson kernel)
1
∫∂Ω|bQ|q dσ . σ(Q)q
∫Q
(kXQ)q dσ(RHweak
q )
. σ(Q)
2
∣∣∣ ∫QbQ dσ
∣∣∣ & σ(Q)ωXQ(Q)[Bourgain]
& σ(Q)
3
∫Q
(SQbQ)q dσ . σ(Q)?
SQbQ(x) =(∫∫
Γ±(x)∩BQ
|∇2SbQ(Y )|2 dY
δ(Y )n−1
) 12
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 20 / 23
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Introduction Main results Strategy of the Proof
Strategy of the Proof: Local Tb for square functions
bQ = σ(Q) ηQ kXQ (normalized and localized Poisson kernel)
1
∫∂Ω|bQ|q dσ . σ(Q)q
∫Q
(kXQ)q dσ(RHweak
q )
. σ(Q)
2
∣∣∣ ∫QbQ dσ
∣∣∣ & σ(Q)ωXQ(Q)[Bourgain]
& σ(Q)
3
∫Q
(SQbQ)q dσ . σ(Q)?
SQbQ(x) =(∫∫
Γ±(x)∩BQ
|∇2SbQ(Y )|2 dY
δ(Y )n−1
) 12
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 20 / 23
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Introduction Main results Strategy of the Proof
Strategy of the Proof: Local Tb for square functions
∇2SbQ(Y )“=”σ(Q)
∫∂Ω∇2Y E(Y − x) dωXQ(x), Y ∈ Γ±(x) ∩BQ
Y ∈ BQ ∩ Ωext
|∇2SbQ(Y )|“=”σ(Q) |∇2Y E(Y−XQ)| . σ(Q) |Y−XQ|−(n+1) . `(Q)−1
Y ∈ BQ ∩ Ω
|∇2SbQ(Y )|“=”σ(Q)∣∣∇2
Y
(E(Y −XQ)−G(Y,XQ)
)∣∣. `(Q)−1 + σ(Q) |∇2
YG(Y,XQ)|∫QSQbQ(x)q dσ(x) . σ(Q) + σ(Q)q
∫QSQu(x)q dσ(x)
SQu(x) =(∫∫
Γ+(x)∩BQ
|∇u(Y )|2 dY
δ(Y )n−1
) 12, u(Y ) = ∇YG(Y,XQ)
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 21 / 23
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Introduction Main results Strategy of the Proof
Strategy of the Proof: Local Tb for square functions
∇2SbQ(Y )“=”σ(Q)
∫∂Ω∇2Y E(Y − x) dωXQ(x), Y ∈ Γ±(x) ∩BQ
Y ∈ BQ ∩ Ωext
|∇2SbQ(Y )|“=”σ(Q) |∇2Y E(Y−XQ)| . σ(Q) |Y−XQ|−(n+1) . `(Q)−1
Y ∈ BQ ∩ Ω
|∇2SbQ(Y )|“=”σ(Q)∣∣∇2
Y
(E(Y −XQ)−G(Y,XQ)
)∣∣. `(Q)−1 + σ(Q) |∇2
YG(Y,XQ)|∫QSQbQ(x)q dσ(x) . σ(Q) + σ(Q)q
∫QSQu(x)q dσ(x)
SQu(x) =(∫∫
Γ+(x)∩BQ
|∇u(Y )|2 dY
δ(Y )n−1
) 12, u(Y ) = ∇YG(Y,XQ)
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 21 / 23
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Introduction Main results Strategy of the Proof
Strategy of the Proof: Local Tb for square functions
∇2SbQ(Y )“=”σ(Q)
∫∂Ω∇2Y E(Y − x) dωXQ(x), Y ∈ Γ±(x) ∩BQ
Y ∈ BQ ∩ Ωext
|∇2SbQ(Y )|“=”σ(Q) |∇2Y E(Y−XQ)| . σ(Q) |Y−XQ|−(n+1) . `(Q)−1
Y ∈ BQ ∩ Ω
|∇2SbQ(Y )|“=”σ(Q)∣∣∇2
Y
(E(Y −XQ)−G(Y,XQ)
)∣∣. `(Q)−1 + σ(Q) |∇2
YG(Y,XQ)|∫QSQbQ(x)q dσ(x) . σ(Q) + σ(Q)q
∫QSQu(x)q dσ(x)
SQu(x) =(∫∫
Γ+(x)∩BQ
|∇u(Y )|2 dY
δ(Y )n−1
) 12, u(Y ) = ∇YG(Y,XQ)
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 21 / 23
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Introduction Main results Strategy of the Proof
Strategy of the Proof: Local Tb for square functions
∇2SbQ(Y )“=”σ(Q)
∫∂Ω∇2Y E(Y − x) dωXQ(x), Y ∈ Γ±(x) ∩BQ
Y ∈ BQ ∩ Ωext
|∇2SbQ(Y )|“=”σ(Q) |∇2Y E(Y−XQ)| . σ(Q) |Y−XQ|−(n+1) . `(Q)−1
Y ∈ BQ ∩ Ω
|∇2SbQ(Y )|“=”σ(Q)∣∣∇2
Y
(E(Y −XQ)−G(Y,XQ)
)∣∣. `(Q)−1 + σ(Q) |∇2
YG(Y,XQ)|∫QSQbQ(x)q dσ(x) . σ(Q) + σ(Q)q
∫QSQu(x)q dσ(x)
SQu(x) =(∫∫
Γ+(x)∩BQ
|∇u(Y )|2 dY
δ(Y )n−1
) 12, u(Y ) = ∇YG(Y,XQ)
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 21 / 23
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Introduction Main results Strategy of the Proof
Strategy of the Proof: Local Tb for square functions
∇2SbQ(Y )“=”σ(Q)
∫∂Ω∇2Y E(Y − x) dωXQ(x), Y ∈ Γ±(x) ∩BQ
Y ∈ BQ ∩ Ωext
|∇2SbQ(Y )|“=”σ(Q) |∇2Y E(Y−XQ)| . σ(Q) |Y−XQ|−(n+1) . `(Q)−1
Y ∈ BQ ∩ Ω
|∇2SbQ(Y )|“=”σ(Q)∣∣∇2
Y
(E(Y −XQ)−G(Y,XQ)
)∣∣. `(Q)−1 + σ(Q) |∇2
YG(Y,XQ)|∫QSQbQ(x)q dσ(x) . σ(Q) + σ(Q)q
∫QSQu(x)q dσ(x)
SQu(x) =(∫∫
Γ+(x)∩BQ
|∇u(Y )|2 dY
δ(Y )n−1
) 12, u(Y ) = ∇YG(Y,XQ)
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 21 / 23
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Introduction Main results Strategy of the Proof
Strategy of the Proof: Local Tb for square functions
∇2SbQ(Y )“=”σ(Q)
∫∂Ω∇2Y E(Y − x) dωXQ(x), Y ∈ Γ±(x) ∩BQ
Y ∈ BQ ∩ Ωext
|∇2SbQ(Y )|“=”σ(Q) |∇2Y E(Y−XQ)| . σ(Q) |Y−XQ|−(n+1) . `(Q)−1
Y ∈ BQ ∩ Ω
|∇2SbQ(Y )|“=”σ(Q)∣∣∇2
Y
(E(Y −XQ)−G(Y,XQ)
)∣∣. `(Q)−1 + σ(Q) |∇2
YG(Y,XQ)|∫QSQbQ(x)q dσ(x) . σ(Q) + σ(Q)q
∫QSQu(x)q dσ(x)
SQu(x) =(∫∫
Γ+(x)∩BQ
|∇u(Y )|2 dY
δ(Y )n−1
) 12, u(Y ) = ∇YG(Y,XQ)
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 21 / 23
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Introduction Main results Strategy of the Proof
Strategy of the Proof: Local Tb for square functions
∇2SbQ(Y )“=”σ(Q)
∫∂Ω∇2Y E(Y − x) dωXQ(x), Y ∈ Γ±(x) ∩BQ
Y ∈ BQ ∩ Ωext
|∇2SbQ(Y )|“=”σ(Q) |∇2Y E(Y−XQ)| . σ(Q) |Y−XQ|−(n+1) . `(Q)−1
Y ∈ BQ ∩ Ω
|∇2SbQ(Y )|“=”σ(Q)∣∣∇2
Y
(E(Y −XQ)−G(Y,XQ)
)∣∣. `(Q)−1 + σ(Q) |∇2
YG(Y,XQ)|∫QSQbQ(x)q dσ(x) . σ(Q) + σ(Q)q
∫QSQu(x)q dσ(x)
SQu(x) =(∫∫
Γ+(x)∩BQ
|∇u(Y )|2 dY
δ(Y )n−1
) 12, u(Y ) = ∇YG(Y,XQ)
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 21 / 23
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Introduction Main results Strategy of the Proof
Strategy of the Proof: Local Tb for square functions
Good-λ inequality a la [Dahlberg-Jerison-Kenig 1984]∫QSQu(x)q dσ(x) .
∫QNQ,∗u(x)q dσ(x), u harmonic BQ ∩ Ω
u(Y ) = ∇YG(Y,XQ), Y ∈ Γ+(x) ∩BQ (harmonic in BQ ∩ Ω)
|u(Y )|Cacciopoli.
G(Y,XQ)
δ(Y )
CFMS≈ ωXQ(∆Y )
σ(∆Y ).M(kXQ χ
Q)(x)
∫QSQu(x)q dσ(x) .
∫Q
(kXQ)q dσ(RHweak
q )
. σ(Q)1−q
∫QSQbQ(x)q dσ(x) . σ(Q) + σ(Q)q
∫QSQu(x)q dσ(x) . σ(Q)
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 22 / 23
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Introduction Main results Strategy of the Proof
Strategy of the Proof: Local Tb for square functions
Good-λ inequality a la [Dahlberg-Jerison-Kenig 1984]∫QSQu(x)q dσ(x) .
∫QNQ,∗u(x)q dσ(x), u harmonic BQ ∩ Ω
u(Y ) = ∇YG(Y,XQ), Y ∈ Γ+(x) ∩BQ (harmonic in BQ ∩ Ω)
|u(Y )|Cacciopoli.
G(Y,XQ)
δ(Y )
CFMS≈ ωXQ(∆Y )
σ(∆Y ).M(kXQ χ
Q)(x)
∫QSQu(x)q dσ(x) .
∫Q
(kXQ)q dσ(RHweak
q )
. σ(Q)1−q
∫QSQbQ(x)q dσ(x) . σ(Q) + σ(Q)q
∫QSQu(x)q dσ(x) . σ(Q)
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 22 / 23
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Introduction Main results Strategy of the Proof
Strategy of the Proof: Local Tb for square functions
Good-λ inequality a la [Dahlberg-Jerison-Kenig 1984]∫QSQu(x)q dσ(x) .
∫QNQ,∗u(x)q dσ(x), u harmonic BQ ∩ Ω
u(Y ) = ∇YG(Y,XQ), Y ∈ Γ+(x) ∩BQ (harmonic in BQ ∩ Ω)
|u(Y )|Cacciopoli.
G(Y,XQ)
δ(Y )
CFMS≈ ωXQ(∆Y )
σ(∆Y ).M(kXQ χ
Q)(x)
∫QSQu(x)q dσ(x) .
∫Q
(kXQ)q dσ(RHweak
q )
. σ(Q)1−q
∫QSQbQ(x)q dσ(x) . σ(Q) + σ(Q)q
∫QSQu(x)q dσ(x) . σ(Q)
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 22 / 23
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Introduction Main results Strategy of the Proof
Strategy of the Proof: Local Tb for square functions
Good-λ inequality a la [Dahlberg-Jerison-Kenig 1984]∫QSQu(x)q dσ(x) .
∫QNQ,∗u(x)q dσ(x), u harmonic BQ ∩ Ω
u(Y ) = ∇YG(Y,XQ), Y ∈ Γ+(x) ∩BQ (harmonic in BQ ∩ Ω)
|u(Y )|Cacciopoli.
G(Y,XQ)
δ(Y )
CFMS≈ ωXQ(∆Y )
σ(∆Y ).M(kXQ χ
Q)(x)
∫QSQu(x)q dσ(x) .
∫Q
(kXQ)q dσ(RHweak
q )
. σ(Q)1−q
∫QSQbQ(x)q dσ(x) . σ(Q) + σ(Q)q
∫QSQu(x)q dσ(x) . σ(Q)
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 22 / 23
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Introduction Main results Strategy of the Proof
Strategy of the Proof: Local Tb for square functions
Good-λ inequality a la [Dahlberg-Jerison-Kenig 1984]∫QSQu(x)q dσ(x) .
∫QNQ,∗u(x)q dσ(x), u harmonic BQ ∩ Ω
u(Y ) = ∇YG(Y,XQ), Y ∈ Γ+(x) ∩BQ (harmonic in BQ ∩ Ω)
|u(Y )|Cacciopoli.
G(Y,XQ)
δ(Y )
CFMS≈ ωXQ(∆Y )
σ(∆Y ).M(kXQ χ
Q)(x)
∫QSQu(x)q dσ(x) .
∫Q
(kXQ)q dσ(RHweak
q )
. σ(Q)1−q
∫QSQbQ(x)q dσ(x) . σ(Q) + σ(Q)q
∫QSQu(x)q dσ(x) . σ(Q)
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 22 / 23
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Introduction Main results Strategy of the Proof
Strategy of the Proof: Local Tb for square functions
Good-λ inequality a la [Dahlberg-Jerison-Kenig 1984]∫QSQu(x)q dσ(x) .
∫QNQ,∗u(x)q dσ(x), u harmonic BQ ∩ Ω
u(Y ) = ∇YG(Y,XQ), Y ∈ Γ+(x) ∩BQ (harmonic in BQ ∩ Ω)
|u(Y )|Cacciopoli.
G(Y,XQ)
δ(Y )
CFMS≈ ωXQ(∆Y )
σ(∆Y ).M(kXQ χ
Q)(x)
∫QSQu(x)q dσ(x) .
∫Q
(kXQ)q dσ(RHweak
q )
. σ(Q)1−q
∫QSQbQ(x)q dσ(x) . σ(Q) + σ(Q)q
∫QSQu(x)q dσ(x) . σ(Q)
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 22 / 23
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Introduction Main results Strategy of the Proof
Strategy of the Proof: Local Tb for square functions
Good-λ inequality a la [Dahlberg-Jerison-Kenig 1984]∫QSQu(x)q dσ(x) .
∫QNQ,∗u(x)q dσ(x), u harmonic BQ ∩ Ω
u(Y ) = ∇YG(Y,XQ), Y ∈ Γ+(x) ∩BQ (harmonic in BQ ∩ Ω)
|u(Y )|Cacciopoli.
G(Y,XQ)
δ(Y )
CFMS≈ ωXQ(∆Y )
σ(∆Y ).M(kXQ χ
Q)(x)
∫QSQu(x)q dσ(x) .
∫Q
(kXQ)q dσ(RHweak
q )
. σ(Q)1−q
∫QSQbQ(x)q dσ(x) . σ(Q) + σ(Q)q
∫QSQu(x)q dσ(x) . σ(Q)
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 22 / 23
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Introduction Main results Strategy of the Proof
Strategy of the Proof: w ∈ Aweak∞ (σ) =⇒ UR
3 UR for Ω
∂ΩN are UR (uniformly in N)
⇓All “nice” SIO are bounded on L2(∂ΩN ) (uniformly in N)
⇓ David’s ideas
All “nice” SIO are bounded on L2(∂Ω)
⇓∂Ω is UR
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 23 / 23
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Introduction Main results Strategy of the Proof
Strategy of the Proof: w ∈ Aweak∞ (σ) =⇒ UR
3 UR for Ω
∂ΩN are UR (uniformly in N)
⇓All “nice” SIO are bounded on L2(∂ΩN ) (uniformly in N)
⇓ David’s ideas
All “nice” SIO are bounded on L2(∂Ω)
⇓∂Ω is UR
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 23 / 23
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Introduction Main results Strategy of the Proof
Strategy of the Proof: w ∈ Aweak∞ (σ) =⇒ UR
3 UR for Ω
∂ΩN are UR (uniformly in N)
⇓All “nice” SIO are bounded on L2(∂ΩN ) (uniformly in N)
⇓ David’s ideas
All “nice” SIO are bounded on L2(∂Ω)
⇓∂Ω is UR
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 23 / 23
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Introduction Main results Strategy of the Proof
Strategy of the Proof: w ∈ Aweak∞ (σ) =⇒ UR
3 UR for Ω
∂ΩN are UR (uniformly in N)
⇓All “nice” SIO are bounded on L2(∂ΩN ) (uniformly in N)
⇓ David’s ideas
All “nice” SIO are bounded on L2(∂Ω)
⇓∂Ω is UR
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 23 / 23
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Introduction Main results Strategy of the Proof
Strategy of the Proof: w ∈ Aweak∞ (σ) =⇒ UR
3 UR for Ω
∂ΩN are UR (uniformly in N)
⇓All “nice” SIO are bounded on L2(∂ΩN ) (uniformly in N)
⇓ David’s ideas
All “nice” SIO are bounded on L2(∂Ω)
⇓∂Ω is UR
J.M. Martell (CSIC) Harmonic Measure and Uniform Rectifiability Toronto, July 2011 23 / 23