Abstract

We investigate the electronic structure of alternating-twist triple Bernal-stacked bilayer graphene (t3BG) as a function of interlayer coupling ωω, twist angle θθ, interlayer potential difference ΔΔ, and top-bottom bilayers sliding vector τ\boldsymbolτ for three possible configurations AB/AB/AB, AB/BA/AB, and AB/AB/BA. The parabolic low-energy band dispersions in a Bernal-stacked bilayer and gap-opening through a finite interlayer potential difference ΔΔ allows the flattening of bands in t3BG down to ∼20\sim 20~meV for twist angles θ≲2∘θ\lesssim 2^{\circ} regardless of the stacking types. The easier isolation of the flat bands and associated reduction of Coulomb screening thanks to the intrinsic gaps of bilayer graphene for finite ΔΔ facilitate the formation of correlation-driven gaps when it is compared to the metallic phases of twisted trilayer graphene under electric fields. We obtain the stacking dependent Coulomb energy versus bandwidth U/W≳1U/W \gtrsim 1 ratios in the θθ and ΔΔ parameter space. We also present the expected KK-valley Chern numbers for the lowest-energy nearly flat bands.

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