Abstract

We present a model of a mechanical system with a vibrational mode spectrum identical to the spectrum of electronic excitations in a tight-binding model of graphene. The model consists of point masses connected by elastic couplings, called ‘tri-bonds’, that implement certain three-body interactions, which can be tuned by varying parameters that correspond to the relative hopping amplitudes on the different bond directions in graphene. In the mechanical model, this is accomplished by varying the location of a pivot point that determines the allowed rigid rotations of a single tri-bond. The infinite system constitutes a Maxwell lattice, with the number of degrees of freedom equal to the number of constraints imposed by the tri-bonds. We construct the equilibrium and compatibility matrices and analyze the model’s phase diagram, which includes spectra with Weyl points for some placements of the pivot and topologically polarized phases for others. We then discuss the edge modes and associated states of self stress for strips cut from the periodic lattice. Finally, we suggest a physical realization of the tri-bond, which allows access to parameter regimes not available to experiments on (strained) graphene and may be used to create other two-dimensional mechanical metamaterials with different spectral features.

Highlights

  • Topology [1,2,3] has become an important tool in advancing our understanding of electronic properties of solids

  • The mechanical model consists of rigid rotors with pivot points fixed on the A-sublattice and connected by central-force springs residing on the the B-sublattice

  • We note that the line in the phase diagram corresponding to x1 = 0 corresponds to a one dimensional limit, in which the system consists of decoupled horizontal lines that are similar to the SSH model

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Summary

INTRODUCTION

Topology [1,2,3] has become an important tool in advancing our understanding of electronic properties of solids. The top and bottom edges of a horizontal strip of the mechanical lattice, which can be created by removing the row of horizontal of dashed tri-bonds in Figure 1 from a periodic lattice, are different: the top surface exposes tri-bond vertices and the bottom a straight continuous line of tri-bond edges These two surfaces correspond, respectively, to the bearded (with dangling bonds) and zigzag edges of graphene [37].

MECHANICAL GRAPHENE MODEL
WEYL POINTS AND PHASE
EDGE STATES
PHYSICAL MODELS
CONCLUDING REMARKS

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