Abstract
van der Waals heterostructures consisting of vertically stacked transition-metal dichalcogenides (TMDs) exhibit a rich landscape of bright and dark intra- and interlayer excitons. In spite of a growing literature in this field of research, the type of excitons dominating optical spectra in different van der Waals heterostructures has not yet been well established. The spectral position of exciton states depends strongly on the strength of hybridization and energy renormalization due to the periodic moir\'e potential. Combining exciton density-matrix formalism and density-functional theory, we shed light on the exciton landscape in TMD homo- and heterobilayers at different stackings. This allows us to identify on a microscopic footing the energetically lowest-lying exciton state for each material and stacking. Furthermore, we disentangle the contribution of hybridization and layer polarization-induced alignment shifts of dark and bright excitons in photoluminescence spectra. By revealing the exciton landscape in van der Waals heterostructures, our work provides the basis for further studies of the optical, dynamical, and transport properties of this technologically promising class of nanomaterials.
Highlights
The emergence of atomically thin semiconductors has opened up a new research venue [1]
By evaluating Eq (7) numerically for different transition metal dichalcogenides (TMDs) bilayers at various temperatures, we reveal the optical footprint of the exciton landscape for different materials at different stackings
We have presented a material specific and fully microscopic model revealing the exciton landscape in TMD homoand heterobilayers at different high-symmetry stackings
Summary
The emergence of atomically thin semiconductors has opened up a new research venue [1]. We analyze the optical footprint of the exciton landscape by calculating photoluminescence (PL) spectra and taking into account direct and phonon-assisted exciton recombination. The latter allows an indirect visualization of dark excitons via the emergence of phonon sidebands [28]. This allows us to identify the microscopic origin of resonances appearing in PL spectra of different TMD homoand heterobilayers at different stackings
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