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Higher order rectifiability via Reifenberg theorems for sets and measures Silvia Ghinassi Stony Brook University March 24, 2019 AMS Spring Spring Central and Western Joint Sectional Meeting Special Session on Topics at the Interface of


  1. Higher order rectifiability via Reifenberg theorems for sets and measures Silvia Ghinassi Stony Brook University March 24, 2019 AMS Spring Spring Central and Western Joint Sectional Meeting Special Session on Topics at the Interface of Analysis and Geometry Silvia Ghinassi (Stony Brook University) Higher order rectifiability via Reifenberg theorems for sets and measures 1 / 21

  2. Parametrizing History ◮ Reifenberg 1960: a “flat” set can be parametrized by a H¨ older map. – The set is required to be flat and without holes: at every point and scale there’s a plane close to the set and the set is close to the plane (official definition coming soon) Silvia Ghinassi (Stony Brook University) Higher order rectifiability via Reifenberg theorems for sets and measures 2 / 21

  3. Parametrizing History ◮ David-Kenig-Toro 2001: a “flat” set with small β numbers can be parametrized by a C 1 ,α map – The sets are “flat” with vanishing constant ◮ Kolasi´ nski 2015: a “flat” set with small holes and small β numbers can be parametrized by a C 1 ,α map – Small holes = size of β – Uses Menger-like curvatures Silvia Ghinassi (Stony Brook University) Higher order rectifiability via Reifenberg theorems for sets and measures 3 / 21

  4. Parametrizing History ◮ David-Toro 2012: a “flat” set with holes can be parametrized by a H¨ older map – Moreover if we assume convergence of a Jones function then we can get a bi-Lipschitz parametrization – No control assumed on the size of the holes Silvia Ghinassi (Stony Brook University) Higher order rectifiability via Reifenberg theorems for sets and measures 4 / 21

  5. Parametrizing The first main theorem (vague statement) ◮ G. 2018: a “flat” set with holes can be parametrized by a C 1 ,α map if we assume a stronger convergence of the Jones function – Again, no control assumed on the size of the holes Silvia Ghinassi (Stony Brook University) Higher order rectifiability via Reifenberg theorems for sets and measures 5 / 21

  6. Parametrizing Definition of Reifenberg flat sets Definition Let E ⊆ R n and let ε > 0. Define E to be Reifenberg flat if the following condition holds. For x ∈ E , 0 < r ≤ 10 there is a d -plane P x , r such that dist( y , P x , r ) ≤ ε r , y ∈ E ∩ B ( x , r ) , dist( y , E ) ≤ ε r , y ∈ P x , r ∩ B ( x , r ) . Moreover we require some compatibility between the P x , r ’s: d x , 10 − k ( P x , 10 − k , P x , 10 − k +1 ) ≤ ε, x ∈ E , d x , 10 − k +2 ( P x , 10 − k , P y , 10 − k ) ≤ ε, x , y ∈ E , | x − y | ≤ 10 − k +2 Silvia Ghinassi (Stony Brook University) Higher order rectifiability via Reifenberg theorems for sets and measures 6 / 21

  7. Parametrizing Definition of one-sided Reifenberg flat sets Definition Let E ⊆ R n and let ε > 0. Define E to be one-sided Reifenberg flat if the following conditions hold. (1) For x ∈ E , 0 < r ≤ 10 there is a d -plane P x , r such that dist( y , P x , r ) ≤ ε r , y ∈ E ∩ B ( x , r ) , dist( y , E ) ≤ ε r , y ∈ P x , r ∩ B ( x , r ) . (2) Moreover we require some compatibility between the P x , r ’s: d x , 10 − k ( P x , 10 − k , P x , 10 − k +1 ) ≤ ε, x ∈ E , d x , 10 − k +2 ( P x , 10 − k , P y , 10 − k ) ≤ ε, x , y ∈ E , | x − y | ≤ 10 − k +2 Silvia Ghinassi (Stony Brook University) Higher order rectifiability via Reifenberg theorems for sets and measures 7 / 21

  8. Parametrizing Definition of β numbers Definition Let E ⊆ R n , x ∈ R n , and r > 0. ◮ β ∞ : dist( y , P ) β E ∞ ( x , r ) = inf sup r P y ∈ E ∩ B ( x , r ) if E ∩ B ( x , r ) � = ∅ , where the infimum is taken over all d -planes P , and β E ∞ ( x , r ) = 0 if E ∩ B ( x , r ) = ∅ . ◮ β p : � p d H d ( y ) � 1 �� � dist( y , P ) p β E p ( x , r ) = inf r d r P E ∩ B ( x , r ) where the infimum is taken over all d -planes P . Silvia Ghinassi (Stony Brook University) Higher order rectifiability via Reifenberg theorems for sets and measures 8 / 21

  9. Parametrizing David-Toro 2012 Theorem (David - Toro, 2012) Let E ⊆ R n be a one-sided Reifenberg flat set. Then we can construct a map f : R d → R n , such that E ⊂ f ( R d ) and f is bi-H¨ older. Moreover, if we assume that there exists M < ∞ such that ∞ ( x , r k ) 2 ≤ M , � β E for all x ∈ E , k ≥ 0 then f is bi-Lipschitz. Silvia Ghinassi (Stony Brook University) Higher order rectifiability via Reifenberg theorems for sets and measures 9 / 21

  10. Parametrizing David-Toro 2012 Theorem (David - Toro, 2012) Let E ⊆ R n be a one-sided Reifenberg flat set. Then we can construct a map f : R d → R n , such that E ⊂ f ( R d ) and f is bi-H¨ older. Moreover, if we assume that there exists M < ∞ such that 1 ( x , r k ) 2 ≤ M , � β E for all x ∈ E , k ≥ 0 then f is bi-Lipschitz. Silvia Ghinassi (Stony Brook University) Higher order rectifiability via Reifenberg theorems for sets and measures 10 / 21

  11. Parametrizing The first main theorem I Theorem (G., 2018) Let E ⊆ R n be a one-sided Reifenberg flat set and α ∈ (0 , 1) . Also assume that there exists M < ∞ such that ∞ ( x , r k ) 2 β E � ≤ M , for all x ∈ E . (1) r 2 α k k ≥ 0 Then we can construct a map f : R d → R n , such that E ⊂ f ( R d ) such that the map and its inverse are C 1 ,α continuous. When α = 1 , if we replace r k in the left hand side of (1) by r k η ( r k ) , where η ( r k ) 2 satisfies the Dini condition, then we obtain that f and its inverse are C 1 , 1 maps. Silvia Ghinassi (Stony Brook University) Higher order rectifiability via Reifenberg theorems for sets and measures 11 / 21

  12. Parametrizing The first main theorem II Theorem (G., 2018) Let E ⊆ R n be a one-sided Reifenberg flat set and α ∈ (0 , 1) . Also assume that there exists M < ∞ such that 1 ( x , r k ) 2 β E � ≤ M , for all x ∈ E . (2) r 2 α k k ≥ 0 Then we can construct a map f : R d → R n , such that E ⊂ f ( R d ) such that the map and its inverse are C 1 ,α continuous. When α = 1 , if we replace r k in the left hand side of (2) by r k η ( r k ) , where η ( r k ) 2 satisfies the Dini condition, then we obtain that f and its inverse are C 1 , 1 maps. Silvia Ghinassi (Stony Brook University) Higher order rectifiability via Reifenberg theorems for sets and measures 12 / 21

  13. Why? ◮ Connection between smoothness and decay of β numbers (applications) ◮ Characterization of rectifiability of measures for different categories (TST type theorems) (Jones, Okikiolu, Schul, David-Semmes, Badger-Schul, Azzam-Tolsa+Tolsa, David-Schul, Li-Schul, Azzam-Schul, Edelen-Naber-Valtorta, Chousionis-Li-Zimmerman, Badger-Naples-Vellis, ...) Silvia Ghinassi (Stony Brook University) Higher order rectifiability via Reifenberg theorems for sets and measures 13 / 21

  14. Rectifiability of measures Theorem (G., 2018) Let µ be a Radon measure on R n such that 0 < θ d ∗ ( µ, x ) < ∞ for µ -a.e. x and α ∈ (0 , 1) . Assume that for µ -a.e. x ∈ R n , 2 ( x , r k ) 2 β µ � J µ 2 ,α ( x ) = < ∞ . (3) r 2 α k k ≥ 0 Then µ is (countably) C 1 ,α d-rectifiable. When α = 1 , if we replace r k in the left hand side of (3) by r k η ( r k ) , where η ( r k ) 2 satisfies the Dini condition, then we obtain that E is C 2 rectifiable. Silvia Ghinassi (Stony Brook University) Higher order rectifiability via Reifenberg theorems for sets and measures 14 / 21

  15. Rectifiability of measures Theorem (G., 2018) Let µ be a Radon measure on R n such that 0 < θ d ∗ ( µ, x ) < ∞ for µ -a.e. x and α ∈ (0 , 1) . Assume that for µ -a.e. x ∈ R n , 2 ( x , r k ) 2 β µ � J µ 2 ,α ( x ) = < ∞ . (3) r 2 α k k ≥ 0 Then µ is (countably) C 1 ,α d-rectifiable. When α = 1 , if we replace r k in the left hand side of (3) by r k η ( r k ) , where η ( r k ) 2 satisfies the Dini condition, then we obtain that E is C 2 rectifiable. (Works with Menger curvatures too! - Kolasi` nski, G.-Goering) Silvia Ghinassi (Stony Brook University) Higher order rectifiability via Reifenberg theorems for sets and measures 14 / 21

  16. A C 1 ,α function which is NOT C 1 ,α + ε � Let h J be the Haar wavelet, normalized so that J | h J ( x ) | dx = 1 � and J h J ( x ) dx = 0, and define � x ψ I ( x ) = h I ( t ) dt −∞ and k � � 2 − α j ψ J ( x ) , g k ( x ) = j =0 J ∈ ∆ j where α ∈ (0 , 1). g ( x ) = lim k →∞ g k ( x ) is a C α function, and so � x 0 g ( t ) dt is a C 1 ,α function. f ( x ) = Silvia Ghinassi (Stony Brook University) Higher order rectifiability via Reifenberg theorems for sets and measures 15 / 21

  17. A C 1 ,α function which is NOT C 1 ,α + ε Figure: The function g k on [0 , 1] for k = 10 and α = 0 . 0001. Silvia Ghinassi (Stony Brook University) Higher order rectifiability via Reifenberg theorems for sets and measures 16 / 21

  18. A C 1 ,α function which is NOT C 1 ,α + ε Figure: The function g k on [0 , 1] for k = 10 and α = 0 . 2. Silvia Ghinassi (Stony Brook University) Higher order rectifiability via Reifenberg theorems for sets and measures 17 / 21

  19. A C 1 ,α function which is NOT C 1 ,α + ε Figure: The function g k on [0 , 1] for k = 10 and α = 0 . 5. Silvia Ghinassi (Stony Brook University) Higher order rectifiability via Reifenberg theorems for sets and measures 18 / 21

  20. A C 1 ,α function which is NOT C 1 ,α + ε Figure: The function g k on [0 , 1] for k = 10 and α = 0 . 8. Silvia Ghinassi (Stony Brook University) Higher order rectifiability via Reifenberg theorems for sets and measures 19 / 21

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