Lattice model for the Coulomb interacting chiral limit of magic-angle twisted bilayer graphene: Symmetries, obstructions, and excitations

We revisit the localized Wannier state description of the twisted bilayer graphene, focusing on the chiral limit. We provide a simple method for constructing such two-dimensional exponentially localized-yet valley polarized-Wannier states, centered on the sites of the honeycomb lattice, paying particular attention to maintaining all the unobstructed symmetries. This includes the unitary particle-hole symmetry, and the combination of C2T and the chiral particle-hole symmetry. The C2T symmetry alone remains topologically obstructed and is not represented in a simple site-to-site fashion. We also analyze the gap and the dispersion of single particle and single hole excitations above a strong coupling ground state at integer fillings, which we find to be dominated by the on-site and the nearest-neighbor terms of a triangular lattice hopping model, with a minimum at the center of the moire Brillouin zone. Finally, we use the insight gained from this real-space description to understand the dependence of the gap and the effective mass on the range of the screened Coulomb interaction.

Automated summary

The study revisits the localized Wannier state description of twisted bilayer graphene, focusing on the chiral limit. It provides a simple method for constructing two-dimensional exponentially localized yet valley-polarized Wannier states while maintaining all unobstructed symmetries. The analysis includes unitary particle-hole symmetry, C2T symmetry, and chiral particle-hole symmetry.