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Twisted bilayer graphene (TBG) hosts a plethora of strongly correlated and topological phases due to its flat bands emerging in the moire superlattice close to the magic angle. However, the effects of the non-Hermiticity, arising from the coupling to the environment and dissipation, have remained unexplored. Here we investigate a possibly simplest non-Hermitian version of twisted bilayer graphene (NH TBG) obtained by relative twisting of two NH graphene monolayers with the non-Hermiticity encoded in imbalance in the in-plane nearest-neighbor hopping amplitudes in the opposite directions. In particular, within the Bistritzer-MacDonald approach generalized to the NH systems, we obtain the corresponding continuum Dirac-like Hamiltonian for the NH TBG, which exhibits two kinds of magic angles. First, it hosts two exceptional magic angles at which the band structure changes from being purely real to purely imaginary, thereby featuring the flat bands in real energy and an infinite lifetime. In between them, the bands remained flattened, and Hermitian magic angle emerges, for which the imaginary part of the energy is maximal and directly corresponds with the usual magic angle in the non-dissipative, purely Hermitian TBG. Our results suggest the robustness of the flat bands in open systems and should motivate studies of the interplay between the non-Hermitian effects and electron interactions in the NH moire bands.
Esparza et al. (Fri,) studied this question.