Geometric combinatorics studies discrete aspects of geometric objects and uses combinatorial methods to prove geometric inequalities.
A Euclidean body is a nonempty bounded measurable subset of of positive Lebesgue measure. Projection inequalities are unchanged by modifying a body on a set of measure zero; geometric equality statements commonly impose additional regularity.
An axis-parallel box in is a Cartesian product of bounded intervals. Its volume is the product of its side lengths, and each coordinate projection is the product of the corresponding intervals.
For , the coordinate projection of consists of the coordinate tuples obtained from points . Its measure is denoted .
A multiset of subsets of is a -uniform cover when every index belongs to exactly members of , counted with multiplicity.
If is a -uniform cover of and is a Euclidean body, then
Slicing in one coordinate, applying the theorem inductively to each slice, and then applying Hölder's inequality to the projected slice functions proves the inequality.
For every Euclidean body , there is an axis-parallel box such that
The proof minimizes an array of candidate projection volumes subject to the finitely many inequalities from irreducible uniform covers. Tight constraints force the array to factor into its singleton coordinates, which become the side lengths of .
The sets form an -uniform cover, so the uniform covers theorem gives
Equality in the three-dimensional Loomis--Whitney inequality forces a measurable body to agree up to a null set with a Cartesian product . This follows from the equality conditions in the two Cauchy-Schwarz inequalities used in its proof. If the body is connected and is a finite union of positive-volume axis-parallel boxes, each is an interval and equality up to a null set upgrades to exact equality with one box.
A uniform cover is irreducible when it is not the disjoint union, as a multiset, of two nonempty uniform covers. There are only finitely many irreducible uniform covers of a fixed finite set: their multiplicity vectors form an antichain in , and Dickson lemma forbids an infinite antichain there.
Every subset of has finitely many coordinatewise minimal elements. Equivalently, has no infinite antichain in its coordinatewise partial order.

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