The measures with $L^2$-bounded Riesz transform and the Painlevé problem
Damian Dąbrowski, Xavier Tolsa
TL;DR
This work provides a precise geometric characterization of measures $\mu$ in $\mathbb{R}^{n+1}$ with polynomial growth for which the $n$-dimensional Riesz transform $R_\mu$ is bounded on $L^2(\mu)$. The authors establish a sharp energy identity linking $\|R_\mu\|_{L^2(\mu)}^2$ to a Wolff-type energy expressed through $β_{2,μ}$ and $θ_μ$, and deduce corollaries on removable sets for Lipschitz harmonic functions and bilipschitz invariance. The approach hinges on a refined David–Mattila lattice, a corona-type decomposition into ${\mathsf{DB}}(M)$-dominated regions, and a novel variational argument on carefully constructed approximating measures supported on tractable trees. By transferring lower bounds from these approximations to the original measure via Haar coefficients, the paper connects geometric density fluctuations to $L^2$-boundedness of singular integrals beyond AD-regular settings. These results advance the Painlevé-type program for Lipschitz harmonic capacities and illuminate the relationship between rectifiability-type geometric quantities and singular integral boundedness in higher codimension.
Abstract
In this work we provide a geometric characterization of the measures $μ$ in $\mathbb R^{n+1}$ with polynomial upper growth of degree $n$ such that the $n$-dimensional Riesz transform $Rμ(x) = \int \frac{x-y}{|x-y|^{n+1}}\,dμ(y)$ belongs to $L^2(μ)$. More precisely, it is shown that $$\|Rμ\|_{L^2(μ)}^2 + \|μ\|\approx \int\!\!\int_0^\infty β_{2,μ}(x,r)^2\,\frac{μ(B(x,r))}{r^n}\,\frac{dr}r\,dμ(x) + \|μ\|,$$ where $β_{μ,2}(x,r)^2 = \inf_L \frac1{r^n}\int_{B(x,r)} \left(\frac{\mathrm{dist}(y,L)}r\right)^2\,dμ(y),$ with the infimum taken over all affine $n$-planes $L\subset\mathbb R^{n+1}$. As a corollary, we obtain a characterization of the removable sets for Lipschitz harmonic functions in terms of a metric-geometric potential and we deduce that the class of removable sets for Lipschitz harmonic functions is invariant by bilipschitz mappings.
