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Minkowski convex-body theorem at equality

Statement

Assume the Axiom of Choice (The Axiom of Choice). Let n≥1, let Λ⊆Rn be a full lattice with covol⁡(Λ)>0 (Full Euclidean lattice and covolume), and let C⊆Rn be compact, convex and centrally symmetric (A convex subset of Rm contains every line segment between two of its points). If

λn(C)≥2ncovol⁡(Λ),

then C contains a nonzero point of Λ.

Facts & Assumptions

Given: The Axiom of Choice, a full lattice Λ with covol⁡(Λ)>0, and a compact convex centrally symmetric C with λn(C)≥2ncovol⁡(Λ).

[A1]

The Axiom of Choice gives the Axiom of Countable Choice (AC implies DC implies countable choice), which licenses the countable selection of one nonzero lattice point vm from each of the sets Sm∩Λ in step 2.1; the strict theorem [F1] and the tiling lemma [F3] are applied under the Axiom of Choice assumed in the statement, and no further choice is used.

[F1]

Strict Minkowski: if a Lebesgue measurable convex centrally symmetric set S satisfies λn(S)>2ncovol⁡(Λ), then S contains a nonzero point of Λ (Minkowski convex-body theorem, strict form).

[F2]

For nonzero real t, λn(tS)=∣t∣nλn(S) for Lebesgue measurable S (For a nonzero real c, dilation by c multiplies Lebesgue outer measure by ∣c∣n, and reflection in the origin preserves it).

[F3]

Every bounded subset of Rn meets Λ in finitely many points (Fundamental parallelotope and finite bounded intersections).

[F4]

C convex: (1−t)x+ty∈C for x,y∈C, t∈[0,1]; C compact, hence closed; central symmetry gives −C=C, so 0∈C since C is nonempty; and for c∈C the convexity relation c/2=12c+12⋅0 gives c/2∈C (A convex subset of Rm contains every line segment between two of its points).

Proof

1.1F2F4given

For every m≥1 the dilate Sm:=(1+1/m)C is compact, convex and centrally symmetric, and by [F2] λn(Sm)=(1+1/m)nλn(C)≥(1+1/m)n2ncovol⁡(Λ)>2ncovol⁡(Λ) because covol⁡(Λ)>0 and (1+1/m)n>1.

2.1A1F1step 1.1

By [F1] each Sm contains a nonzero lattice point; using [A1] choose one, say 0≠vm∈Sm∩Λ, for every m≥1.

3.1F3F4step 2.1

Since 1+1/m≤2 for m≥1 and 0∈C, convexity of C gives Sm⊆2C, so every vm lies in the bounded set 2C; by [F3] the set 2C∩Λ is finite, so some v∈2C∩Λ equals vm for infinitely many m.

4.1F4step 3.1

Fix such an infinite set of indices m. For each of them v∈(1+1/m)C, hence v/(1+1/m)∈C; as m→∞ through those indices v/(1+1/m)→v, and C is closed by [F4], so v∈C.

5.1step 4.1∎

The point v is nonzero by step 2.1 and lies in C∩Λ, so C contains a nonzero lattice point.

Remarks

Compactness is used twice: it makes 2C∩Λ finite and it makes C closed, so that the limit of the points v/(1+1/m) stays in C. For non-closed bodies the conclusion can fail: the open cube (−1,1)n has λn=2ncovol⁡(Zn) and meets Zn only in the origin.

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