Heterogeneous stacks of two-dimensional transition-metal dichalcogenides can be arranged so as to have a type-II band alignment, where the valence band maximum and the conduction band minimum are located on different layers. These structures can host long-living interlayer excitons with inhibited charge recombination and enhanced charge-carrier separation. Interlayer excitons appear as photoluminescence peaks below the band gap, but not in absorption experiments, indicating that they may form after and not during absorption. In order to quantify the interlayer component of the absorption spectra of such heterostructures, we perform first-principles calculations of the layer-decomposed dielectric function of the ${\mathrm{HfS}}_2/{\mathrm{PtS}}_2$ heterobilayer. This has a type-II band alignment and a relatively small interlayer distance, which should facilitate the formation of interlayer excitons. We find that the interlayer component is always only a small fraction of the total dielectric function, owing to the large spatial separation between the electron and the hole. However, the interlayer contribution is greatly enhanced upon reducing the interlayer distance. Compression of the layers produces a split-off band at the top of the valence bands. This remains localized on ${\mathrm{PtS}}_2$ so that the heterostructure preserves the type-II character. At the same time the type-II bandgap is reduced, moving the interlayer absorption peak to a lower energy and to a position well separated from the rest of the absorption spectrum.

• Received 18 September 2019

DOI:https://doi.org/10.1103/PhysRevMaterials.3.124002