English

Layer potentials for elliptic operators with DMO-type coefficients: big pieces $Tb$ theorem, quantitative rectifiability, and free boundary problems

Analysis of PDEs 2025-05-30 v1 Classical Analysis and ODEs

Abstract

For n2n \geq 2, we consider the operator LA=div(A())L_A = -\mathrm{div }(A(\cdot)\nabla), where AA is a uniformly elliptic (n+1)×(n+1)(n+1)\times(n+1) matrix with variable coefficients, a Radon measure μ\mu on Rn+1\mathbb{R}^{n+1}, and the associated gradient of the single layer potential operator TμT_\mu. Under a Dini-type assumption on the mean oscillation of the matrix AA, we establish the following results: 1) A rectifiability criterion for μ\mu in terms of TμT_\mu. Under quantitative geometric and analytic assumptions within a ball BB -- including an upper nn-growth condition on μ\mu in BB, a thin boundary condition, a scale-invariant decay condition expressed via a weighted sum of densities over dyadic dilations of BB, and L2L^2 boundedness of the gradient of TμT_\mu -- we show the following: if the support of μ\mu lies very close to an nn-plane in BB, and Tμ1T_\mu 1 is nearly constant on BB in the L2L^2 sense, then there exists a uniformly nn-rectifiable set Γ\Gamma such that μ(BΓ)μ(B)\mu(B \cap \Gamma) \gtrsim \mu(B). 2) A TbTb theorem for suppressed TμT_\mu, which extends a well-known theorem of Nazarov, Treil, and Volberg, and holds also for a broader class of singular integral operators. These results make it possible to prove both qualitative and quantitative one- and two-phase free boundary problems for elliptic measure, formulated in terms of (uniform) rectifiability, in bounded Wiener-regular domains.

Keywords

Cite

@article{arxiv.2505.23478,
  title  = {Layer potentials for elliptic operators with DMO-type coefficients: big pieces $Tb$ theorem, quantitative rectifiability, and free boundary problems},
  author = {Andrea Merlo and Mihalis Mourgoglou and Carmelo Puliatti},
  journal= {arXiv preprint arXiv:2505.23478},
  year   = {2025}
}

Comments

80 pages

R2 v1 2026-07-01T02:48:29.285Z