Global Rigidity: The Effect of Coning

  • Authors:
  • R. Connelly;W. J. Whiteley

  • Affiliations:
  • Cornell University, Department of Mathematics, 14853, Ithaca, NY, USA;York University, Department of Mathematics and Statistics, 4700 Keele Street, M3J 1P3, Toronto, ON, Canada

  • Venue:
  • Discrete & Computational Geometry
  • Year:
  • 2010

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Abstract

Recent results have confirmed that the global rigidity of bar-and-joint frameworks on a graph G is a generic property in Euclidean spaces of all dimensions. Although it is not known if there is a deterministic algorithm that runs in polynomial time and space, to decide if a graph is generically globally rigid, there is an algorithm (Gortler et al. in Characterizing generic global rigidity, arXiv:0710.0907v1, 2007) running in polynomial time and space that will decide with no false positives and only has false negatives with low probability. When there is a framework that is infinitesimally rigid with a stress matrix of maximal rank, we describe it as a certificate which guarantees that the graph is generically globally rigid, although this framework, itself, may not be globally rigid. We present a set of examples which clarify a number of aspects of global rigidity. There is a technique which transfers rigidity to one dimension higher: coning. Here we confirm that the cone on a graph is generically globally rigid in ℝd+1 if and only if the graph is generically globally rigid in ℝd . As a corollary, we see that a graph is generically globally rigid in the d-dimensional sphere $\mathbb{S}^{d}$if and only if it is generically globally rigid in ℝd .