English

On rectifiable measures in Carnot groups: Marstrand-Mattila rectifiability criterion

Metric Geometry 2022-02-28 v1

Abstract

In this paper we continue the study of the notion of P\mathscr{P}-rectifiability in Carnot groups. We say that a Radon measure is Ph\mathscr{P}_h-rectifiable, for hNh\in\mathbb N, if it has positive hh-lower density and finite hh-upper density almost everywhere, and, at almost every point, it admits a unique tangent measure up to multiples. In this paper we prove a Marstrand--Mattila rectifiability criterion in arbitrary Carnot groups for P\mathscr{P}-rectifiable measures with tangent planes that admit a normal complementary subgroup. Namely, in this co-normal case, even if a priori the tangent planes at a point might not be the same at different scales, a posteriori the measure has a unique tangent almost everywhere. Since every horizontal subgroup of a Carnot group has a normal complement, our criterion applies in the particular case in which the tangents are one-dimensional horizontal subgroups. Hence, as an immediate consequence of our Marstrand--Mattila rectifiability criterion and a result of Chousionis--Magnani--Tyson, we obtain the one-dimensional Preiss's theorem in the first Heisenberg group H1\mathbb H^1. More precisely, we show that a Radon measure ϕ\phi on H1\mathbb H^1 with positive and finite one-density with respect to the Koranyi distance is absolutely continuous with respect to the one-dimensional Hausdorff measure H1\mathcal{H}^1, and it is supported on a one-rectifiable set in the sense of Federer, i.e., it is supported on the countable union of the images of Lipschitz maps from ARA\subseteq \mathbb R to H1\mathbb H^1.

Keywords

Cite

@article{arxiv.2202.12741,
  title  = {On rectifiable measures in Carnot groups: Marstrand-Mattila rectifiability criterion},
  author = {Gioacchino Antonelli and Andrea Merlo},
  journal= {arXiv preprint arXiv:2202.12741},
  year   = {2022}
}

Comments

This is the second of two companion papers derived from arXiv:2009.13941v2. The present work consists of an elaboration of Sections 2 and 5 of the Preprint 2009.13941v2, while the first of the two (that will appear as 2009.13941v3) is an elaboration of Sections 2, 3, 4, and 6 of 2009.13941v2

R2 v1 2026-06-24T09:53:58.822Z