Kondo effect in twisted bilayer graphene

The emergence of flat bands in twisted bilayer graphene at the magic angle can be understood in terms of a vanishing Fermi velocity of the Dirac cone. This is associated with van Hove singularities approaching the Fermi energy and becoming higher-order. In the density of states, this is reflected by flanking logarithmic van Hove divergences pinching off the central Dirac cone in energy space. The low-energy pseudogap of the Dirac cone away from the magic angle is replaced by a power-law divergence due to the higher-order van Hove singularity at the magic angle. This plays an important role in the exotic phenomena observed in this material, such as superconductivity and magnetism, by amplifying electronic correlation effects. Here we investigate one such correlation effect-the Kondo effect due to a magnetic impurity embedded in twisted bilayer graphene. We use the Bistritzer-MacDonald model to extract the low-energy density of states of the material as a function of twist angle and study the resulting quantum impurity physics using perturbative and numerical renormalization group methods. Although at zero temperature the impurity is only Kondo screened precisely at the magic angle, we find highly nontrivial behavior at finite temperatures relevant to experiments, due to the complex interplay between Dirac, van Hove, and Kondo physics.

Automated summary

The emergence of flat bands in twisted bilayer graphene at the magic angle can be understood as a result of vanishing Fermi velocity of the Dirac cone and higher-order van Hove singularities. These characteristics play an important role in exotic phenomena observed in this material, such as superconductivity and magnetism, by enhancing electronic correlation effects. One of these correlation effects is the Kondo effect due to a magnetic impurity embedded in twisted bilayer graphene. The interplay between Dirac, van Hove, and Kondo physics leads to nontrivial behavior at finite temperatures relevant to experiments.