Let E⊂R2 be a planar set. The Favard length of E is defined by
Fav(E) := π1∫0π∣ProjRθE∣dθ,
where Proj is orthogonal projection to the horizontal axis and Rθ is rotation by angle θ.
[NPV2011-def-fav]
The Favard length has the following probabilistic interpretation: up to a constant factor, Fav(E) is the probability that a “Buffon’s needle” (a long line segment dropped at random) hits E.
[NPV2011-buffon-interpretation]
Let Cn be the n-th stage in the construction of the middle-half Cantor set, and let
Kn := Cn×Cn.
Then Kn is a union of 4n axis-parallel squares of side length 4−n.
[NPV2011-Kn-4n-squares]
A classical theorem of Besicovitch implies that Fav(Kn)→0 as n→∞, and it remains open to determine the exact rate of decay.
[NPV2011-besicovitch-open-decay]
We define the Favard-length decay exponent αFav by
C60 := αFav := sup{α≥0: ∃C>0 such that Fav(Kn)≤Cn−α for all n∈N}.
The best established range currently is
61 ≤ αFav ≤ 1.
[NPV2011-thm1-powerlaw] [BV2010-thm1-lb-logn-over-n]