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7 - Sections, section functions, and point X-rays

Published online by Cambridge University Press:  05 June 2013

Richard J. Gardner
Affiliation:
Western Washington University
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Summary

The various themes explored in earlier chapters have both synthesis and counterpoint in this one. Just as Chapter 3 examined inverse problems where the given data involve orthogonal projections, so this chapter deals with information about sections through one or more points.

Much of the first section mirrors Section 3.1. Though star bodies would be the natural objects to consider, we have had to retreat to convexity for lack of more general results. For example, Theorem 7.1.9 implies that two convex bodies in En, n ≥ 3, must be homothetic if their intersections with any hyperplane through the origin are also homothetic. In the realm of convex bodies, a useful duality is provided by polar bodies (see Section 0.8). Via (0.38), this sometimes enables one to convert a theorem concerning projections to one about sections through the origin, or vice versa. We apply this technique in Theorem 7.1.11, which shows that “homothetic” cannot be replaced by “similar” in the foregoing statement. Unfortunately polar duality is of limited relevance in geometric tomography (cf. the last paragraph of Section 0.8), and we can only apply it on a couple of occasions. This means that separate proofs usually have to be constructed, even when there is a direct analogy with a result in Chapter 3. Moreover, the “mirror” is imperfect; for example, Theorem 7.1.9 actually draws the stronger conclusion that the bodies must either be dilatates or homothetic ellipsoids. Similarly, Theorem 7.1.10, sometimes called the false center theorem, states that if the intersection of a convex body with any hyperplane through the origin is centrally symmetric, the body must either be centered or an ellipsoid.

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Chapter
Information
Geometric Tomography , pp. 269 - 303
Publisher: Cambridge University Press
Print publication year: 2006

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