Theory of Optical Activity in Doped Systems with Application to Twisted Bilayer Graphene
arXiv:2210.03960 · doi:10.1103/PhysRevB.106.245405
Abstract
We theoretically study the optical activity in a doped system and derive the optical activity tensor from a light wavevector-dependent linear optical conductivity. Although the light-matter interaction is introduced through the velocity gauge from a minimal coupling Hamiltonian, we find that the well-known ``false divergences'' problem can be avoided in practice if the electronic states are described by a finite band effective Hamiltonian, such as a few-band tight-binding model. The expression we obtain for the optical activity tensor is in good numerical agreement with a recent theory derived for an undoped topologically trivial gapped system. We apply our theory to the optical activity of a gated twisted bilayer graphene, with a detailed discussion of the dependence of the results on twist angle, chemical potential, gate voltage, and location of rotation center forming the twisted bilayer graphene.
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Cited by in corpus (8)
- Multipole theory of optical spatial dispersion in crystals
- Flat-band optical phonons in twisted bilayer graphene
- Optical activity and transport in twisted bilayer graphene: the essence of spatial dispersion effects
- Intrinsic and extrinsic photogalvanic effects in twisted bilayer graphene
- Layer Hall counterflow as a model probe of magic-angle twisted bilayer graphene
- Unique properties of the optical activity in noncentrosymmetric superconductors: sum rule, missing area, and relation with the superconducting Edelstein effect
- Shift current response in twisted double bilayer graphenes
- Orbital optical activity in noncentrosymmetric metals and superconductors