Abstract

The classification of materials into insulators and conductors has been shaken up by the discovery of topological insulators that conduct robustly at the edge but not in the bulk. In mechanics, designating a material as insulating or conducting amounts to asking if it is rigid or floppy. Although mechanical structures that display topological floppy modes have been proposed, they are all vulnerable to global collapse. Here, we design and build mechanical metamaterials that are stable and yet capable of harboring protected edge and bulk modes, analogous to those in electronic topological insulators and Weyl semimetals. To do so, we exploit gear assemblies that, unlike point masses connected by springs, incorporate both translational and rotational degrees of freedom. Global structural stability is achieved by eliminating geometrical frustration of collective gear rotations extending through the assembly. The topological robustness of the mechanical modes makes them appealing across scales from engineered macrostructures to networks of toothed microrotors of potential use in micro-machines.

Highlights

  • The classification of materials into insulators and conductors has been shaken up by the discovery of topological insulators that conduct robustly at the edge but not in the bulk

  • Mechanisms often underlie the behavior of mechanical metamaterials—artificial structures whose mechanical properties arise from the geometry and arrangement of their building blocks [8,9]

  • First introduced in isostatic spring networks [16,17,18], topological mechanical modes are insensitive to a wide range of structural perturbations like their counterparts in electronics [19,20], photonics [21], and acoustics [22,23,24,25,26,27,28,29]

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Summary

Introduction

The classification of materials into insulators and conductors has been shaken up by the discovery of topological insulators that conduct robustly at the edge but not in the bulk. To find Maxwell gear networks with a spectral gap and nontrivial topology [nonzero winding numbers of CðkÞ], we consider modifications of the martini lattice [45], which has four sites and six links per unit cell on a regular hexagonal Bravais lattice (see Appendix B for descriptions of all lattices used in this work).

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