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Semiconductor moiré materials with strong spin-orbit coupling

This project investigates the effects of moiré superlattices (Fig. 1a and 1b) in van der Waals homo- and heterobilayers based on semiconducting transition metal dichalcogenides, in particular MoSe₂, WSe₂, and WS₂. Moiré superlattices arise in these structures due to differences in the lattice constants of the individual layers and/or a non-zero twist angle between them (Fig. 1a).

In selenide-based heterostructures (e.g., MoSe₂/WSe₂), atomic reconstruction occurs in both untwisted and small-angle twisted configurations. In contrast, sulfide–selenide heterobilayers (e.g., MoSe₂/WS₂) exhibit moiré superlattices even without twisting due to their larger lattice mismatch.

To experimentally investigate these systems, we employ low-frequency resonant Raman spectroscopy (e.g., Fig. 1c), continuous-wave and time-resolved photoluminescence, as well as time-resolved pump-probe spectroscopy.

Fig. 1 | (a) Schematic representation of a twisted MoSe2 homobilayer. The green arrows and the green shaded area mark the moiré supercell, while the red arrows outline the crystallographic supercell. (b) Hexagonal Brillouin zone of layer 1 with reciprocal basis vectors b1 and b2 of the two twisted layers 1 and 2. g is the reciprocal lattice vector of the moiré superlattice. (c) Low-frequency Raman spectra of a series of twisted MoSe2 homobilayers. The small arrows mark Moiré phonons.

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