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Cylindrical Partitions of Convex Bodies

Published online by Cambridge University Press:  27 June 2025

Jacob E. Goodman
Affiliation:
City College, City University of New York
Janos Pach
Affiliation:
City College, City University of New York and New York University
Emo Welzl
Affiliation:
Eidgenössische Technische Hochschule Zürich
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Summary

A cylindrical partition of a convex body in ℝn is a partition of the body into subsets of smaller diameter, obtained by intersecting the body with a collection of mutually parallel convex-base cylinders. Convex bodies of constant width are characterized as those that do not admit a cylindrical partition. The main result is a finite upper bound, exponential in n, on the minimum number bc(n)of pieces needed in a cylindrical partition of every convex body of nonconstant width in Rn. (A lower bound on bc(n), exponential in, is a consequence of the construction of Kalai and Kahn for counterexamples to Borsuk's conjecture.) We also consider cylindrical partitions of centrally symmetric bodies and of bodies with smooth boundaries.

1. Introduction and Preliminaries

Throughout this article, M denotes a compact subset of ℝn containing at least two points. By diamM we denote the maximum distance between points of M, but diameter of M also means the line segment connecting any pair of points of M that realize this distance (ambiguity is always avoided by the context). A Borsuk partition of M is a family of subsets of M, each of diameter smaller than diamM, whose union contains M. The Borsuk partition number of M, denoted by b(M), is the minimum number of sets needed in a Borsuk partition of M. It is obvious that b(M) is finite. It is also obvious that the maximum of b(M) over all bounded sets M in ℝn exists and is bounded above exponentially in n, since every set of diameter d is contained in a ball of radius d.

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Publisher: Cambridge University Press
Print publication year: 2005

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