Emergent Localization in Dodecagonal Bilayer Quasicrystals
arXiv:1812.09170 · doi:10.1103/PhysRevB.99.245401
Abstract
A new type of long-range ordering in the absence of translational symmetry gives rise to drastic revolution of our common knowledge in condensed matter physics. Quasicrystal, as such unconventional system, became a plethora to test our insights and to find exotic states of matter. In particular, electronic properties in quasicrystal have gotten lots of attention along with their experimental realization and controllability in twisted bilayer systems. In this work, we study how quasicrystalline order in bilayer systems can induce unique localization of electrons without any extrinsic disorders. We focus on dodecagonal quasicrystal that has been demonstrated in twisted bilayer graphene system in recent experiments. In the presence of small gap, we show the localization generically occurs due to non-periodic nature of quasicrystal, which is evidenced by the inverse participation ratio and the energy level statistics. We understand the origin of such localization by approximating the dodecagonal quasicrystals as an impurity scattering problem.
4 pages, 5 figures
References in corpus (10)
- Localization of interacting fermions at high temperature
- Continuum Model of the Twisted Bilayer
- Modeling disorder in graphene
- Numerical studies of confined states in rotated bilayers of graphene
- Localization and Kosterlitz-Thouless Transition in Disordered Graphene
- Low energy theory of disordered graphene
- Interlayer interaction in general incommensurate atomic layers
- Quasicrystalline electronic states in 30 rotated twisted bilayer graphene
- Anderson localization of electron states in graphene in different types of disorder
- Anderson localization transitions with and without random potentials