Definition

Let 0<ν10<\nu\le 1 and 0<α0<α10<\alpha_0<\alpha_1. A set YRdY\subseteq\mathbb R^d is ν\nu-porous on lines from scales α0\alpha_0 to α1\alpha_1 if, for every line segment τ\tau of length RR with α0<R<α1\alpha_0<R<\alpha_1, some xτx\in\tau satisfies

BνR(x)Y=.B_{\nu R}(x)\cap Y=\varnothing.

The missing ball may extend away from the line, but its center must lie on the tested segment.

Why this is stronger than ball porosity

Every line-porous set is , after an inessential adjustment of constants. The converse fails for d2d\ge2: a straight line has large holes inside ambient balls but has none along segments lying in that line. Line porosity therefore excludes orthogonal linear concentrations that obstruct higher-dimensional uncertainty estimates.

Stability properties

Dilating YY by s>0s>0 multiplies both endpoint scales by ss and preserves ν\nu. Intersecting with any fixed line produces a one-dimensional porous set. A sufficiently small remains line porous with a smaller porosity constant and a larger lower scale.

References
  1. Alex Cohen, “Fractal uncertainty in higher dimensions,” 2024. arXiv record. Relevant: §§1.2 and A.2.