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Strong Coupling Theory of Magic-Angle Graphene: A Pedagogical Introduction

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arxiv 2105.08858 v2 pith:EOVERLBY submitted 2021-05-19 cond-mat.str-el cond-mat.mes-hall

classification cond-mat.str-elcond-mat.mes-hall
keywords couplingapproachgraphenestrongtheorybandseffectivefillings
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abstract

We give a self contained review of a recently developed strong coupling theory of magic-angle graphene. An advantage of this approach is that a single formulation can capture both the insulating and superconducting states, and with a few simplifying assumptions, can be treated analytically. We begin by reviewing the electronic structure of magic angle graphene's flat bands, in a limit that exposes their peculiar band topology and geometry. We highlight how similarities between the flat bands and the lowest Landau level give insight into the effect of interactions. For example, at certain fractional fillings, we note the promise for realizing fractional Chern states. At integer fillings, this approach points to flavor ordered insulators, which can be captured by a sigma-model in its ordered phase. Unexpectedly, topological textures of the sigma model carry electric charge which allows us to extend the same theory to describe the doped phases away from integer filling. We show how this approach can lead to superconductivity on disordering the sigma model, and estimate the T$_c$ for the superconductor. We highlight the important role played by an effective super-exchange coupling both in pairing and in setting the effective mass of Cooper pairs. Seeking to enhance this coupling helps predict new superconducting platforms, including the recently discovered alternating twist trilayer platform. We also contrast our proposal from strong coupling theories for other superconductors.

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  1. Mixed valence Mott insulator and composite excitation in twisted bilayer graphene

    cond-mat.str-el 2025-06 conditional novelty 5.0 of 10

    At ν=-2, twisted bilayer graphene is argued to host a mixed valence Mott insulator where the f orbital is a superposition of f2+ and f3+, with a low-energy composite excitation near Γ.

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