A square function involving the center of mass and rectifiability

preprint2022arXivOpen access

Abstract

For a Radon measure μμ on Rd\mathbb{R}^d, define Cμn(x,t)= (1tn ∣∫B(x,t)x−yt dμ(y) ∣ )C^n_μ(x, t)= \ (\frac{1}{t^n} \ |\int_{B(x,t)} \frac{x-y}{t} \, dμ(y)\ | \ ). This coefficient quantifies how symmetric the measure μμ is by comparing the center of mass at a given scale and location to the actual center of the ball. We show that if μμ is nn-rectifiable, then $ \int_0^\infty |C^n_μ(x,t)|^2 \frac{dt}{t} < \infty \, \, μ\mbox{-almost everywhere}. $ Together with a previous result of Mayboroda and Volberg, where they showed that the converse holds true, this gives a characterisation of nn-rectifiability. To prove our main result, we also show that for an nn-uniformly rectifiable measure, ∣Cμn(x,t)∣2dt/tdμ|C_μ^n(x,t)|^2 dt/t dμ is a Carleson measure on spt(μ)×(0,∞)\mathrm{spt}(μ) \times (0,\infty). We also show that, whenever a measure μμ is 11-rectifiable in the plane, then the same Dini condition as above holds for more general kernels. Moreover, we give a characterisation of uniform 1-rectifiability in the plane in terms of a Carleson measure condition.

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