Searcharxiv⌕ Search

arXiv · 0706.2958

On the shadow boundary of a centrally symmetric convex body

Abstract

We discuss the concept of the shadow boundary of a centrally symmetric convex ball $K$ (actually being the unit ball of a Minkowski normed space) with respect to a direction ${\bf x}$ of the Euclidean n-space $R^n$. We introduce the concept of general parameter spheres of $K$ corresponding to this direction and prove that the shadow boundary is a topological manifold if all of the non-degenerated general parameter spheres are, too. In this case, using the approximation theorem of cell-like maps we get that they are homeomorphic to the $(n-2)$-dimensional sphere $S^{(n-2)}$. We also prove that the bisector (equidistant set of the corresponding normed space) in the direction ${\bf x}$ is homeomorphic to $R^{(n-1)}$ iff all of the non-degenerated general parameter spheres are $(n-2)$-manifolds implying that if the bisector is a homeomorphic copy of $R^{(n-1)}$ then the corresponding shadow boundary is a topological $(n-2)$-sphere.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

Akos G. Horvath. 2007-06-20. On the shadow boundary of a centrally symmetric convex body. https://arxiv.org/abs/0706.2958

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

Divide and Conquer: A Distributed Approach to Five Point Energy Minimization

This work rigorously verifies the phase transition in 5-point energy minimization first observed by Melnyk-Knop-Smith in 1977. More precisely, we prove that there is a constant S = [15+24/512,15+25/512] such that the triangular bi-pyramid is the energy minimizer with respect to the s-power law potential for all s in (0,S) and some pyramid with square base is the unique minimizer for all s in (S,15+512/25]. Taking s=1 gives another solution to Thomson's 5 electron problem from 1904.

math.MG↗

Quadri-Figures in Cayley-Klein Planes II: The Miquel-Steiner Theorem

The Miquel-Steiner theorem for a quadrilateral in the euclidean plane states that the circumcircles of the four component triangles intersect at a single point, which now is called the Miquel-Steiner point of the quadrilateral. The Miquel-Steiner theorem for euclidean planes needs to be slightly modified for Minkowski and galilean planes: Either the circumcircles of the four component triangles touch each other at an isotropic point, or they intersect transversally at an anisotropic point. In elliptic and hyperbolic planes, as well as in dual euclidean and dual Minkowski planes, Miquel-Steiner's theorem does not hold in this form. Instead, a weaker version applies: The circumcircles of the four component triangles of a quadrilateral have a common radical center, which we will also call the Miquel-Steiner point. For specific quadrilaterals (such as cyclic quadrilaterals), the location of the Miquel-Steiner point can be determined more precisely.

math.MG↗

The Four Color Theorem meets Shapes of Polyhedra

We consider solutions to the $4$-color problem for the vertices of sphere triangulations with degree sequence $6,...,6,4,4,4,4,4,4$. We sort these solutions into combinatorial types and show that each generic type $τ$ is parametrized by the set of integer lattice points inside a rational polyhedral convex cone ${\cal C\/}_τ$ of dimension at least 4. There is an integral quadratic form $Q_τ$ on ${\cal C\/}_τ$ whose diagonal part, evaluated on a lattice point, is $3$ times the number of triangles in the corresponding triangulation. We relate this structure to the octahedral stratum of Thurston's moduli space of flat cone structures on the sphere.

math.MG↗