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  • Letter

Non-Abelian effective mechanism from layer pseudospin and lattice pseudospin in twisted bilayer graphene

Zheng Liu1, Chao Zhang2,3,*, and J. C. Cao1,†

  • 1Key Laboratory of Terahertz Solid-State Technology, Shanghai Institute of Microsystem and Information Technology, Chinese Academy of Sciences, 865 Changning Road, Shanghai 200050, China
  • 2School of Physics, University of Wollongong, New South Wales 2522, Australia
  • 3Institute of Superconducting and Electronic Materials, University of Wollongong, New South Wales 2522, Australia

  • *czhang@uow.edu.au
  • †jccao@mail.sim.ac.cn

Phys. Rev. B 104, L041403 – Published 12 July, 2021

DOI: https://doi.org/10.1103/PhysRevB.104.L041403

Abstract

In the work by Tarnopolsky et al. [Phys. Rev. Lett. 122, 106405 (2019)] they obtained the magic angles for superconductivity in twisted bilayer graphene (TBG) with a fundamental continuum model for TBG which captures the physics of the flat band. In this Letter we study the continuum model in detail and demonstrate that the system of TBG described by the continuum model is equivalent to a dynamical system that is composed of three parts of effective interactions: the coupling between two effective non-Abelian gauge fields originating from the periodic hopping potential and two effective massless fermion fields which have 1/2 lattice pseudospin and a twist-angle-dependent effective charge, the coupling between a pseudomagnetic field created by gauge fields and a layer pseudospin, and an effective pseudo-Rashba effect in an equivalent unrotated single layer with twist-angle-dependent Rashba coupling strength. The effective Rashba effect is shown to be also the sum of the pseudo-Rashba effects in two effective twisted single layers with a relative twist angle π−θ. The longitudinal component τ̂z of the layer pseudospin vector is revealed to have the physical meaning of an interlayer electric field. Due to the relative twist between the two layers it geometrically leads to the nonvanishing curvature on a vector bundle in a two-dimensional effective hexagonal lattice. The geometric curvature on the vector bundle creates a pseudomagnetic field physically and interacts with the layer pseudospin.

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