Abstract

We compute the energy spectrum of a nearest-neighbor electron hopping model for bi-layer graphene at commensurate twist angles. Specifically, we focus on the simplest bi-layer lattices, with moiré patterns that have no subcells. The electron hopping hamiltonian is analyzed in momentum space, both by degenerate perturbation theory and by exact numerical calculation. We find that the degeneracy in energy along the edge of the moiré Brillouin zone due to the two valley quantum numbers is noticeably broken in the flat central bands at the magic twist angle. A mechanism for the appearance of flat central bands themselves at the magic twist angle is also revealed. It is due to maximal level repulsion. The mechanism relies on the assumption that the phase factor for the AA hamiltonian matrix element for inter-graphene-sheet hopping at the middle of the edge of the moiré Brillouin zone has a phase equal to half the twist angle. This assumption is confirmed in the case of uniform AA hopping in between the two sheets of graphene, in the limit of large moiré unit cells.

Abstract

We compute the energy spectrum of a nearest-neighbor electron hopping model for bi-layer graphene at commensurate twist angles. Specifically, we focus on the simplest bi-layer lattices, with moiré patterns that have no subcells. The electron hopping hamiltonian is analyzed in momentum space, both by degenerate perturbation theory and by exact numerical calculation. We find that the degeneracy in energy along the edge of the moiré Brillouin zone due to the two valley quantum numbers is noticeably broken in the flat central bands at the magic twist angle. A mechanism for the appearance of flat central bands themselves at the magic twist angle is also revealed. It is due to maximal level repulsion. The mechanism relies on the assumption that the phase factor for the AA hamiltonian matrix element for inter-graphene-sheet hopping at the middle of the edge of the moiré Brillouin zone has a phase equal to half the twist angle. This assumption is confirmed in the case of uniform AA hopping in between the two sheets of graphene, in the limit of large moiré unit cells.

Abstract

We compute the energy spectrum of a nearest-neighbor electron hopping model for bi-layer graphene at commensurate twist angles. Specifically, we focus on the simplest bi-layer lattices, with moiré patterns that have no subcells. The electron hopping hamiltonian is analyzed in momentum space, both by degenerate perturbation theory and by exact numerical calculation. We find that the degeneracy in energy along the edge of the moiré Brillouin zone due to the two valley quantum numbers is noticeably broken in the flat central bands at the magic twist angle. A mechanism for the appearance of flat central bands themselves at the magic twist angle is also revealed. It is due to maximal level repulsion. The mechanism relies on the assumption that the phase factor for the AA hamiltonian matrix element for inter-graphene-sheet hopping at the middle of the edge of the moiré Brillouin zone has a phase equal to half the twist angle. This assumption is confirmed in the case of uniform AA hopping in between the two sheets of graphene, in the limit of large moiré unit cells.

Abstract

We compute the energy spectrum of a nearest-neighbor electron hopping model for bi-layer graphene at commensurate twist angles. Specifically, we focus on the simplest bi-layer lattices, with moiré patterns that have no subcells. The electron hopping hamiltonian is analyzed in momentum space, both by degenerate perturbation theory and by exact numerical calculation. We find that the degeneracy in energy along the edge of the moiré Brillouin zone due to the two valley quantum numbers is noticeably broken in the flat central bands at the magic twist angle. A mechanism for the appearance of flat central bands themselves at the magic twist angle is also revealed. It is due to maximal level repulsion. The mechanism relies on the assumption that the phase factor for the AA hamiltonian matrix element for inter-graphene-sheet hopping at the middle of the edge of the moiré Brillouin zone has a phase equal to half the twist angle. This assumption is confirmed in the case of uniform AA hopping in between the two sheets of graphene, in the limit of large moiré unit cells.