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Gruber P. Convex and Discrete Geometry

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210 <strong>Convex</strong> Bodies<br />

Theorem 11.4. Let C ∈ Cp be of class C2 with Gauss curvature κC > 0. Then there<br />

is a constant δ = δ2,d−1 > 0, depending only on d, such that<br />

(1) δ V (C, P c ⎛<br />

�<br />

δ<br />

(n) ) ∼ ⎝ κC(x)<br />

2<br />

1<br />

⎞ d+1<br />

d−1<br />

d+1 dσ(x) ⎠<br />

1<br />

as n →∞.<br />

bd C<br />

n 2<br />

d−1<br />

Here, σ is the ordinary surface area measure on bd C. The integral in the asymptotic<br />

formula (1) is the affine surface area of C, a notion from affine differential geometry.<br />

It is invariant with respect to volume preserving affinities of the convex body C.The<br />

constant δ = δ2,d−1 was introduced in [427], where we wrote div (for Dirichlet<br />

<strong>and</strong> Voronoĭ) instead of δ. It is related to Dirichlet–Voronoĭ tilings, see Sect. 32.1.<br />

We have,<br />

δ2,2 = 5<br />

18 √ 3 , δ2,d−1∼ d<br />

as d →∞.<br />

2πe<br />

For the value of δ2,2, see Fejes Tóth [329] <strong>and</strong> the author [425, 427]. For a proof of<br />

the asymptotic formula for δ2,d−1, see Proposition 33.1.<br />

Proof. Let λ>1. We start with some preparations. For p ∈ bd C, letH be the<br />

unique support hyperplane of C at p. Choose a Cartesian coordinate system in H<br />

with origin at p. Together with the interior unit normal vector of bd C at p, itforms<br />

a Cartesian coordinate system in E d . The lower part of bd C with respect to the last<br />

coordinate then can be represented in the form:<br />

� s, f (s) � : s ∈ C ′ ,<br />

where “ ′ ” denotes the orthogonal projection of Ed onto H <strong>and</strong> f is a convex function<br />

on C ′ such that f | relint C ′ is of class C2 .Foru∈ relint C ′ , define the quadratic form<br />

qu = qpu by<br />

qu(s) = �<br />

fxi ,x j (u)sisj for s = (s1,...,sd−1) ∈ H.<br />

i, j<br />

Let qp = qpp. The Gauss curvature κC(u) at the point x = � u, f (u) � ∈ bd C,<br />

u ∈ relint C ′ , is then given by<br />

κC(u) =<br />

det qu<br />

� � � . d+1 2�<br />

1 + grad f (u) 2<br />

We also write κC(x) for κC(u). Since κC > 0, the quadratic forms qu are all positive<br />

definite. Since f is of class C 2 , their coefficients are continuous. Hence we may<br />

choose an open convex neighbourhood U ′ ⊆ C ′ of p in H such that<br />

1<br />

λ qp(s) ≤ qu(s) ≤ λqp(s) for s ∈ H, u ∈ U ′<br />

1<br />

λ det qp ≤ det qu ≤ λ det qp for u ∈ U ′<br />

1<br />

λ κC(u) ≤ det qp ≤ λκC(u) for u ∈ U ′

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