Magic angle conditions for twisted three-dimensional topological insulators

We derive a general low-energy theory for twisted moiré heterostructures comprised of Dirac materials. We apply our theory to heterostructures on the surface of a three-dimensional topological insulator (3D TI). First, we consider the interface between two 3D TIs arranged with a relative twist angle. We prove that if the two TIs are identical, then a necessary condition for a perturbative magic angle where the Dirac cone velocity vanishes is to have an interlayer spin-flipping hopping term. Without this term, the Dirac cone velocities can still be significantly renormalized, decreasing to less than half of their original values, but they will not vanish. Second, we consider graphene on the surface of a TI arranged with a small twist angle. Again, a magic angle is unachievable with only a spin-flipping hopping term; under such conditions, the Dirac cone is renormalized, but only moderately. In both cases, our perturbative results are verified by computing the band structure of the continuum model. The enhanced density of states that results from decreasing the surface Dirac cone velocity provides a tunable route to realizing interacting topological phases.