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Gruber P. Convex and Discrete Geometry

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If<br />

22 Minkowski’s First Fundamental Theorem 371<br />

V (Eϱ) = ϱ d 2 V (B d )<br />

det(aik) 1 .<br />

2<br />

�<br />

det(aik)<br />

ϱ = 4<br />

V (B d ) 2<br />

� 1<br />

d<br />

,<br />

then V (Eϱ) = 2 d . Now apply the fundamental theorem to the convex body Eϱ <strong>and</strong><br />

the lattice Z d . ⊓⊔<br />

For smaller upper estimates, but in the terminology of density of packings<br />

of balls, see Sect. 29.2 <strong>and</strong> the articles of Blichfeldt, Sidel’nikov, Levenstein <strong>and</strong><br />

Kabat’janskiĭ cited there. The best known upper bound is that of Levenstein <strong>and</strong><br />

Kabat’janskiĭ.<br />

Minkowski’s Linear Form Theorem<br />

This result can be formulated as follows, see Minkowski [735]:<br />

Corollary 22.2. Let l1,...,ld be d real linear forms in d real variables, such that the<br />

absolute value δ of their determinant is positive. Assume further that τ1,...,τd > 0<br />

are such that τ1 ···τd ≥ δ. Then the following system of inequalities has a non-trivial<br />

integer solution<br />

|l1(x)| ≤τ1,...,|ld(x)| ≤τd.<br />

Proof. Apply the fundamental theorem to the parallelotope P <strong>and</strong> the lattice Z d ,<br />

where<br />

P = � � 2<br />

x :|l1(x)| ≤τ1,...,|ld(x)| ≤τd , V (P) = dτ1 ···τd<br />

δ<br />

≥ 2 d . ⊓⊔<br />

The estimate in the linear form theorem cannot be improved for all systems of linear<br />

forms.<br />

Simultaneous Diophantine Approximation<br />

As a consequence of the linear form theorem, we obtain a classical approximation<br />

result due to Kronecker [618]. He proved it by means of Dirichlet’s pigeon hole<br />

principle. Here, we follow Minkowski [735] who used his linear form theorem.<br />

Corollary 22.3. Let ϑ1,...,ϑd ∈ R. Then the following system of inequalities has<br />

infinitely many integer solutions (u0, u1,...,ud), where u0 �= 0:<br />

�<br />

�<br />

�ϑ1 − u1<br />

�<br />

�<br />

� ≤ 1<br />

u0<br />

u 1+ 1 d<br />

0<br />

�<br />

�<br />

,..., �ϑd − ud<br />

�<br />

�<br />

� ≤ 1<br />

u0<br />

u 1+ 1 d<br />

0<br />

.

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