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Local Poincaré constants and mean oscillation functionals for $BV$ functions

Adolfo Arroyo-Rabasa, Paolo Bonicatto, Giacomo Del Nin

Abstract

We introduce the concept of local Poincaré constant of a $BV$ function as a tool to understand the relation between its mean oscillation and its total variation at small scales. This enables us to study a variant of the BMO-type seminorms on $\varepsilon$-size cubes introduced by Ambrosio, Bourgain, Brezis, and Figalli. More precisely, we relax the size constraint by considering a family of functionals that allow cubes of sidelength smaller than or equal to $\varepsilon$. These new functionals converge, as $\varepsilon$ tends to zero, to a local functional defined on $BV$, which can be represented by integration in terms of the local Poincaré constant and the total variation. This contrasts with the original functionals, whose limit is defined on $SBV$ and may not exist for functions with a non-trivial Cantor part. Moreover, we characterize the local Poincaré constant of a function with a cell-formula given by the maximum mean oscillation of its $BV$ blow-ups. As a corollary of this characterization, we show that the new limit functional extends the original one to all $BV$ functions. Finally, we discuss rigidity properties and other challenging questions relating the local Poincaré constant of a function to its fine properties.

Local Poincaré constants and mean oscillation functionals for $BV$ functions

Abstract

We introduce the concept of local Poincaré constant of a function as a tool to understand the relation between its mean oscillation and its total variation at small scales. This enables us to study a variant of the BMO-type seminorms on -size cubes introduced by Ambrosio, Bourgain, Brezis, and Figalli. More precisely, we relax the size constraint by considering a family of functionals that allow cubes of sidelength smaller than or equal to . These new functionals converge, as tends to zero, to a local functional defined on , which can be represented by integration in terms of the local Poincaré constant and the total variation. This contrasts with the original functionals, whose limit is defined on and may not exist for functions with a non-trivial Cantor part. Moreover, we characterize the local Poincaré constant of a function with a cell-formula given by the maximum mean oscillation of its blow-ups. As a corollary of this characterization, we show that the new limit functional extends the original one to all functions. Finally, we discuss rigidity properties and other challenging questions relating the local Poincaré constant of a function to its fine properties.
Paper Structure (22 sections, 34 theorems, 169 equations, 4 figures)

This paper contains 22 sections, 34 theorems, 169 equations, 4 figures.

Key Result

Theorem 1.1

There exists a dimensional constant $\tau(n) \in (0,1)$ with the following property: if $f \in BV_\mathrm{loc}(\Omega)$, then for all $\tau(n) \le \tau < 1$.

Figures (4)

  • Figure 1: The shaded area depicts the $\tau$-contraction $\tau Q_i$ of each cube $Q_i$ ($i = 1,2,3$). Only $Q_2$ and $Q_3$ are admissible for $P_f^\tau(x,\varepsilon)$.
  • Figure 2: An oriented cube $Q\subset \mathbb{R}^2$. The vectors $b_1-x_Q$ and $b_2-x_Q$ are orthogonal.
  • Figure 3: The function $j=j_{a,b,\nu,c}$ of Lemma \ref{['lemma:tangents_of_SBV']} (in 2d). The function $j$ takes constant values $a,b$ and jumps from value $a$ to $b$ across the line $H_{\nu,c}$.
  • Figure 4: On the left: on the interval $I_1$ of scale $r_i^{-1}k_i^{-1}$ the function is close to a jump. On the right: on the interval $I_2$ of intermediate scale $r_i^{-1}$ the function looks affine.

Theorems & Definitions (67)

  • Theorem 1.1
  • Theorem 1.2
  • Theorem 1.3
  • Corollary 1.4
  • Corollary 1.5
  • Proposition 2.1
  • proof
  • Remark 2.2
  • Lemma 3.1
  • proof
  • ...and 57 more