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Gruber P. Convex and Discrete Geometry

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6 Mixed Volumes <strong>and</strong> Quermassintegrals 97<br />

pn(λ1,...,λd) → p(λ1,...,λd) as n →∞<br />

for each d-tuple λ1,...,λd ≥ 0.<br />

Assume that all coefficients ai1...idn <strong>and</strong> ai1...id of pn <strong>and</strong> p, respectively,<br />

are symmetric in their indices i1,...,id. Then<br />

ai1...id n → ai1...id for all i1,...,id ∈{1,...,d}.<br />

To show the theorem, consider sequences (C1n), . . . , (Cdn) in C converging to<br />

C1,...,Cd ∈ C say, respectively. Since for λ1,...,λd ≥ 0, we have λ1C1n +···+<br />

λdCdn → λ1C1 +···+λdCd, the continuity of volume, which will be proved in<br />

Theorem 7.5, yields<br />

V (λ1C1n +···+λdCdn) → V (λ1C1 +···+λdCd)<br />

for λ1,...,λd ≥ 0.<br />

Now apply Minkowski’s mixed volume Theorem 6.5 <strong>and</strong> the above remark for<br />

a12...dn = V (C1n,...,Cdn) <strong>and</strong> a12...d = V (C1,...,Cd). ⊓⊔<br />

Monotony<br />

Mixed volumes are non-decreasing in their entries.<br />

Theorem 6.9. Let C1,...,Cd, D1,..., Dd ∈ C such that C1 ⊆ D1,...,Cd ⊆ Dd.<br />

Then V (C1,...,Cd) ≤ V (D1,...,Dd).<br />

As examples show, equality does not mean that necessarily Ci = Di for all i. The<br />

proof of the theorem is based on several lemmas which are of interest themselves.<br />

Let v(·) denote (d −1)-dimensional volume. (For (d −1)-dimensional polytopes <strong>and</strong><br />

thus for facets of d-dimensional polytopes it coincides with elementary area measure<br />

for polytopes, see Sect. 16.1.)<br />

Lemma 6.4. Let C ∈ C <strong>and</strong> P ∈ P. For each facet F of P let u F be the exterior unit<br />

normal vector of F. Then<br />

(3) V (C, P,...,P) = 1 �<br />

hC(u F)v(F).<br />

d<br />

F facet of P<br />

Proof. First, the following will be shown:<br />

(4) Let G be a face of P with dim G ≤ d − 2. Then<br />

V (G + εB d ) = O(ε 2 ) as ε →+0.<br />

We may assume that G ⊆ E d−2 , where E d is represented in the form E d = E d−2 ×<br />

E 2 .LetB d−2 , B 2 be the corresponding unit balls. Choose ϱ>0 so large that G +<br />

εB d−2 ⊆ ϱB d−2 for 0 < ε ≤ 1. Then G + εB d ⊆ (G + εB d−2 ) × εB 2 ⊆<br />

ϱB d−2 × εB 2 <strong>and</strong> thus V (G + εB d ) = O(ε 2 ) as ε →+0.

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