This analysis discovers RG flows impacting Coulomb and Hubbard interactions in magic-angle twisted bilayer graphene, indicating implications for Kondo-like and Mott-semimetal scenarios.
We develop a perturbative renormalization group (RG) theory for the topological heavy fermion (THF) model, describing magic-angle twisted bilayer graphene (MATBG) as an emergent Anderson lattice. The realistic parameters place MATBG near an intermediate regime where the Hubbard interaction U and the hybridization energy $γ$ are comparable, motivating the need for RG analysis. Our approach analytically tracks the flow of single-particle parameters and Coulomb interactions within an energy window below $0.1$ eV, providing implications for distinguishing between Kondo-like (U γ) and projected-limit/Mott-semimetal (U γ) scenarios at low energies. We show that the RG flows generically lower the ratio $U/γ$ and drive MATBG toward the chiral limit, consistent with the previous numerical study based on the Bistritzer-MacDonald model. The framework presented here also applies to other moiré systems and stoichiometric materials that admit a THF description, including magic-angle twisted trilayer graphene, twisted checkerboard model, and Lieb lattice, among others, providing a foundation for developing low-energy effective theories relevant to a broad class of topological flat-band materials.
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Huang et al. (2025) studied this question.
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