Projection body
In convex geometry, the projection body of a convex body
in n-dimensional Euclidean space is the convex body such that for any vector
, the support function of
in the direction u is the (n , 1)-dimensional volume of the projection of K onto the hyperplane orthogonal to u.
Hermann Minkowski showed that the projection body of a convex body is convex. Petty (1967) and Schneider (1967) used projection bodies in their solution to Shephard's problem.
For a convex body, let
denote the polar body of its projection body. There are two remarkable affine isoperimetric inequality for this body. Petty (1971) proved that for all convex bodies
,
where denotes the n-dimensional unit ball and
is n-dimensional volume, and there is equality precisely for ellipsoids. Zhang (1991) proved that for all convex bodies
,
where denotes any
-dimensional simplex, and there is equality precisely for such simplices.
The intersection body IK of K is defined similarly, as the star body such that for any vector u the radial function of IK from the origin in direction u is the (n , 1)-dimensional volume of the intersection of K with the hyperplane u⊥. Equivalently, the radial function of the intersection body IK is the Funk transform of the radial function of K. Intersection bodies were introduced by Lutwak (1988).
Koldobsky (1998a) showed that a centrally symmetric star-shaped body is an intersection body if and only if the function 1/||x|| is a positive definite distribution, where ||x|| is the homogeneous function of degree 1 that is 1 on the boundary of the body, and Koldobsky (1998b) used this to show that the unit balls lp
n, 2 < p ≤ ∞ in n-dimensional space with the lp norm are intersection bodies for n=4 but are not intersection bodies for n ≥ 5.
Sources and credits
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