Abstract

Dodecagonal bilayer graphene quasicrystal has 12-fold rotational order but lacks translational symmetry which prevents the application of band theory. In this paper, we study the electronic and optical properties of graphene quasicrystal with large-scale tight-binding calculations involving more than ten million atoms. We propose a series of periodic approximants which reproduce accurately the properties of quasicrystal within a finite unit cell. By utilizing the band-unfolding method on the smallest approximant with only 2702 atoms, the effective band structure of graphene quasicrystal is derived. The features, such as the emergence of new Dirac points (especially the mirrored ones), the band gap at M point and the Fermi velocity are all in agreement with recent experiments. The properties of quasicrystal states are identified in the Landau level spectrum and optical excitations. Importantly, our results show that the lattice mismatch is the dominant factor determining the accuracy of layered approximants. The proposed approximants can be used directly for other layered materials in honeycomb lattice, and the design principles can be applied for any quasi-periodic incommensurate structures.

Highlights

  • The bilayer graphene with van der Waals interlayer interaction shows rich electronic properties that are depending on the stacking order and twist angle.[1,2,3,4,5,6,7,8,9,10,11,12,13,14,15]

  • The 12-fold rotational symmetry has been determined by the Raman spectroscopy, low-energy electron microscopy/diffraction (LEEM/LEED), transmission electron microscopy (TEM) and scanning tunneling microscopy (STM) measurements.[21,22,23,24,25]

  • Angle-resolved photoemission spectroscopy (ARPES) measurements indicated that the interlayer interaction between the two layers leads to the emergence of the mirrorsymmetric Dirac cones inside the Brillouin zone of each graphene layer[21,22,23] and a gap opening at the zone boundary.[23]

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Summary

INTRODUCTION

The bilayer graphene with van der Waals interlayer interaction shows rich electronic properties that are depending on the stacking order and twist angle.[1,2,3,4,5,6,7,8,9,10,11,12,13,14,15] Two graphene layers can be arranged in AA, AB or twisted configurations. We construct the approximant in the following way: the twist angle of 30 is fixed and the top graphene layer is compressed or stretched to satisfy the condition M 3b 1⁄4 Nat, where at is the lattice constant of the top graphene layer with strain This method was point arithmetic which corresponds to 8 bytes for a real number applied to construct the periodic structure to calculate the and 16 bytes for a complex number.

Yu et al 3
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