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Gruber P. Convex and Discrete Geometry

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The First Fundamental Theorem<br />

22 Minkowski’s First Fundamental Theorem 367<br />

A very satisfying answer to the above problem is the following first fundamental<br />

theorem of Minkowski [734] or Minkowski’s first theorem:<br />

Theorem 22.1. Let C be an o-symmetric convex body <strong>and</strong> L a lattice in E d such that<br />

V (C) ≥ 2 d d(L). Then C contains a pair of points ±l ∈ L \{o}.<br />

The first proof is based on Dirichlet’s pigeon hole principle <strong>and</strong> a formula to<br />

calculate the volume of a convex body. The idea to use the pigeon hole principle<br />

in this context seems to be due to Scherrer [886]. The second proof is due to Siegel<br />

[935] <strong>and</strong> makes use of Fourier series <strong>and</strong> Parseval’s theorem. The third one utilizes a<br />

close relation between the fundamental theorem <strong>and</strong> the notion of density of a lattice<br />

packing of convex bodies (Fig. 22.1).<br />

Proof (using the pigeon hole principle). Since C is compact <strong>and</strong> L discrete, it is<br />

sufficient to prove the theorem under the stronger assumption that<br />

(1) V (C) >2 d d(L).<br />

The convex body 1 2C is Jordan measurable by Theorem 7.4. Using the substitution<br />

rule for multiple integrals, the asymptotic formula (3) in Sect. 7.2 to calculate the<br />

Jordan measure then implies that<br />

�<br />

1<br />

V<br />

2 C<br />

� �<br />

1 1<br />

∼ # C ∩<br />

2 n L<br />

� �<br />

1<br />

· d<br />

n L<br />

�<br />

as n →∞.<br />

Since by (1) V ( 1 2C)>d(L), it follows that<br />

�<br />

1 1<br />

(2) # C ∩<br />

2 n L<br />

�<br />

> n d for all sufficiently large n.<br />

Keep such an n fixed <strong>and</strong> choose a basis {b1,...,bd} of L. To each point<br />

u1<br />

n b1 +···+ ud<br />

n bd ∈ 1 1<br />

C ∩<br />

2 n L<br />

Cd<br />

o<br />

Fig. 22.1. Fundamental theorem

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