Statement

Let XRdX\subseteq\mathbb R^d be ν\nu- from scales α0\alpha_0 to α1\alpha_1. There are constants C,γ>0C,\gamma>0, depending only on ν\nu and dd, such that every ball BB of radius RR with α0<R<α1\alpha_0<R<\alpha_1 satisfies

XBCRd(α0R)γ.|X\cap B|\le C R^d\left(\frac{\alpha_0}{R}\right)^\gamma.
Mechanism

Choose an LL-adic grid with Ldν1L\asymp_d\nu^{-1}. gives , so at every admissible depth at least one child of each occupied cube is empty. Iterating the factor 1Ld1-L^{-d} through Nlog(R/α0)N\asymp\log(R/\alpha_0) levels gives the power saving.

Quantitative exponent

One may choose γ\gamma comparable from below to νd/logν\nu^d/|\log\nu|, with a dimension-dependent constant. Sharpness of this particular expression is not asserted.

References
  1. Alex Cohen, “Fractal uncertainty in higher dimensions,” 2024. arXiv record. Relevant: Lemmas A.6–A.7.