In mathematics, the affine plank problem is an open question in convex geometry posed by Thøger Bang in 1951 as a strengthening of Tarski's plank problem. It a
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In mathematics, the affine plank problem is an open question in convex geometry posed by Thøger Bang in 1951 as a strengthening of Tarski's plank problem. It asks whether the sum of the relative widths of any collection of planks covering a convex body must be at least 1. Unlike the original plank problem, which was solved by Bang himself, the affine plank problem remains open in general, although it has been resolved for special cases including centrally symmetric bodies.[1]
The problem is also known as Bang's conjecture,[2] the affine plank conjecture,[3] or the affine-invariant plank problem;[4] sometimes described as a geometric pigeonhole principle.[1]
A plank in is the closed region between two parallel hyperplanes. Given a convex body (a compact convex set with nonempty interior) and a plank with unit normal vector , the relative width of with respect to is
where is the width of the plank (the distance between its bounding hyperplanes) and is the width of in the direction (the distance between the two supporting hyperplanes of perpendicular to ).
Conjecture (Bang, 1951)—If planks cover a convex body , then
Since for every direction , the relative width of any plank is at most its absolute width divided by the minimal width of . Therefore, the affine plank conjecture implies Bang's theorem (the solution to Tarski's plank problem), making it a strictly stronger statement.[2]
A key feature of relative width is its affine invariance: if is an invertible affine transformation, then the relative width of with respect to equals the relative width of with respect to . This invariance is the reason for the name "affine plank problem".[5]
Alexander (1968) showed that the affine plank conjecture is equivalent to a geometric generalisation of the pigeonhole principle:[6]
Conjecture (equivalent form)—Given a convex body in and hyperplanes, there exists a translate of inside whose interior does not meet any of the hyperplanes.
Ball (1991) described this as a "multi-dimensional pigeon-hole principle".[1] The equivalence connects the affine plank problem to Diophantine approximation via observations of Harold Davenport (1962).[6][7]
The most important partial result is due to Ball (1991), who proved the conjecture for centrally symmetric convex bodies.[1] Ball reformulated the problem in terms of Banach spaces: every centrally symmetric convex body can serve as the unit ball of a finite-dimensional Banach space, and the conjecture becomes the statement that if the unit ball is covered by planks, the sum of their half-widths (relative to the norm) is at least 1. Ball extended this result to infinite-dimensional Banach spaces in the same paper.
Ball's proof reduces the problem to a statement about matrices with 1s on the diagonal, then uses an orthogonal change of basis to symmetrize the matrix so that Bang's lemma can be applied. This approach also yielded a complex plank theorem for Hilbert spaces.[8]
Bang proved the conjecture for the case of two planks in 1953, with alternative proofs later given by Alexander (1968) and Gardner (1988).[6][9][2]
The conjecture remains open in the plane: Bang's 1953 result covers only coverings by two planks, not arbitrary coverings in .[3] Even the case of three planks on a triangle is unsettled.[2]
Akopyan, Karasev, and Petrov (2019) proved the conjecture in the case where all planks have one of two normal directions, using techniques from symplectic geometry.[10]
For general convex bodies, the best known unconditional lower bounds on the sum of relative widths are:
In the plane (), the Bakaev–Yehudayoff bound gives approximately 0.828. Their proof uses the support function and John's position of the difference body , combined with an inequality relating chord length to width for convex bodies inscribed between concentric balls.[3]
Ambrus (2010) showed that the affine plank conjecture for planks on all convex bodies in all dimensions reduces to verifying it for the regular -simplex.[5] The argument proceeds by choosing, for each plank direction, a pair of points in that realise the width, then expressing the covering condition in terms of barycentric coordinates on a simplex formed by these points. This reduction means, for example, that proving the conjecture for three planks on the 5-dimensional simplex would imply it for three planks on any convex body in any dimension.
Through its connections to Bang's lemma and its equivalent formulations, the affine plank problem and its partial solutions have applications in several areas:
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