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Gruber P. Convex and Discrete Geometry

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172 <strong>Convex</strong> Bodies<br />

Proposition 9.2. Let C ∈ Cp be o-symmetric. Then, Steiner symmetrization, with<br />

respect to a given hyperplane through o, satisfies the following inequality:<br />

V � (st C) ∗� ≥ V (C ∗ ).<br />

Proof. We may suppose that this hyperplane is E d−1 ={x : xd = 0}. Then<br />

st C = �� x, 1<br />

2 (s − t)� : (x, r), (x, s) ∈ C � ,<br />

C ∗ = � (y, t) : x · y + st ≤ 1for(x, s) ∈ C � ,<br />

(st C) ∗ = � (w, t) : x · w + 1<br />

2 (r − s)t ≤ 1for(x, r), (x, s) ∈ C� .<br />

For a set A ⊆ E d <strong>and</strong> t ∈ R, letA(t) ={v ∈ E d−1 : (v, t) ∈ A}. Then<br />

1�<br />

�<br />

∗ ∗<br />

C (t) + C (−t)<br />

2<br />

= �1<br />

(y + z) : x · y + rt ≤ 1, w· z + s(−t) ≤ 1for(x, r), (w, s) ∈ C�<br />

2<br />

⊆ �1<br />

(y + z) : x · y + rt ≤ 1, x · z + s(−t) ≤ 1for(x, r), (x, s) ∈ C�<br />

2<br />

⊆ �1<br />

2<br />

(y + z) : x · 1<br />

2<br />

1<br />

(y + z) + (r − s)t ≤ 1for(x, r), (x, s) ∈ C�<br />

2<br />

= � w : x · w + 1<br />

(r − s)t ≤ 1for(x, r), (x, s) ∈ C�<br />

2<br />

= (st C) ∗ (t) for t ∈ R.<br />

Since C is o-symmetric, C∗ is also o-symmetric. Thus C∗ (t) =−C∗ (−t) <strong>and</strong> therefore<br />

v � C∗ (t) � = v � C∗ (−t) � . The Brunn–Minkowski inequality in d − 1 dimensions<br />

then shows that<br />

v � (st C) ∗ (t) � �<br />

1�<br />

� ∗ ∗<br />

≥ v C (t) + C (−t) �<br />

≥<br />

2<br />

�<br />

1<br />

2 v�C ∗ � 1 1<br />

(t) d−1 +<br />

2 v� C ∗ (−t)<br />

� 1 �d−1 d−1<br />

= v � C ∗ (t) � for t ∈ R.<br />

Now, integrating over t, Fubini’s theorem yields V � (st C) ∗� ≥ V (C ∗ ). ⊓⊔<br />

The Sphericity Theorem of Gross<br />

The following highly intuitive sphericity theorem of Gross [407] <strong>and</strong> its corollary<br />

were used by Blaschke [124] for easy proofs of the isodiametric, the isoperimetric<br />

<strong>and</strong> the Brunn–Minkowski inequalities. Let κd = V (B d ).<br />

Theorem 9.1. Let C ∈ Cp with V (C) = V (B d ). Then, there is a sequence<br />

C1, C2,...of convex bodies, each obtained from C by finitely many successive<br />

Steiner symmetrizations with respect to hyperplanes through o, such that<br />

C1, C2, ···→ B d .

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