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Rigidity of symmetric simplicial complexes and the lower bound theorem

Published online by Cambridge University Press:  20 January 2025

James Cruickshank
Affiliation:
School of Mathematical and Statistical Sciences, University of Galway, University Road, Galway, H91 TK33, Ireland; E-mail: james.cruickshank@universityofgalway.ie
Bill Jackson*
Affiliation:
School of Mathematical Sciences, Queen Mary University of London, Mile End Road, London, E1 4NS, United Kingdom
Shin-ichi Tanigawa
Affiliation:
Department of Mathematical Informatics, University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo, 113-8654, Japan; E-mail: tanigawa@mist.i.u-tokyo.ac.jp
*
E-mail: b.jackson@qmul.ac.uk (corresponding author)

Abstract

We show that if $\Gamma $ is a point group of $\mathbb {R}^{k+1}$ of order two for some $k\geq 2$ and $\mathcal {S}$ is a k-pseudomanifold which has a free automorphism of order two, then either $\mathcal {S}$ has a $\Gamma $-symmetric infinitesimally rigid realisation in ${\mathbb R}^{k+1}$ or $k=2$ and $\Gamma $ is a half-turn rotation group. This verifies a conjecture made by Klee, Nevo, Novik and Zheng for the case when $\Gamma $ is a point-inversion group. Our result implies that Stanley’s lower bound theorem for centrally symmetric polytopes extends to pseudomanifolds with a free simplicial automorphism of order 2, thus verifying (the inequality part of) another conjecture of Klee, Nevo, Novik and Zheng. Both results actually apply to a much larger class of simplicial complexes – namely, the circuits of the simplicial matroid. The proof of our rigidity result adapts earlier ideas of Fogelsanger to the setting of symmetric simplicial complexes.

Information

Type
Discrete Mathematics
Creative Commons
Creative Common License - CCCreative Common License - BY
This is an Open Access article, distributed under the terms of the Creative Commons Attribution licence (https://creativecommons.org/licenses/by/4.0/), which permits unrestricted re-use, distribution, and reproduction in any medium, provided the original work is properly cited.
Copyright
© The Author(s), 2025. Published by Cambridge University Press
Figure 0

Figure 1 The Bricard octahedron.

Figure 1

Figure 2 The 1-skeleton of a $\mathbb Z_2$-irreducible $2$-cycle $\mathcal {S}$, which is not a simplicial 2-circuit. We have $\mathcal {S}=\mathcal {T}\sqcup \mathcal {T}^*$, where $\mathcal {T}=\{\{v_1,v_2,v_3\},\{v_1,v_2,v_4\},\{v_1,v_3,v_4\},\{v_1^*,v_2,v_3\},\{v_1^*,v_2,v_4\},\{v_1^*,v_3,v_4\}\}$ is the simplicial 2-circuit given by the boundary complex of the hexahedron.