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Probing Evolution of Twist-Angle-Dependent Interlayer Excitons in MoSe<sub>2</sub>/WSe<sub>2</sub> van der Waals Heterostructures
308
Citations
57
References
2017
Year
Oxide HeterostructuresSemiconductorsTransition Metal ChalcogenidesInterlayer ExcitonsEngineeringPhysicsLayered MaterialSurface ScienceApplied PhysicsCondensed Matter PhysicsQuantum MaterialsInterlayer SeparationExcitonic PhenomenaMultilayer HeterostructuresOptoelectronic DevicesHeterostructuresTopological HeterostructuresTwist-angle-dependent Interlayer Excitons
Interlayer excitons have been observed at van der Waals heterostructure junctions, but the influence of stacking order on these excitonic phenomena remains unknown. We investigate twist‑angle‑dependent interlayer excitons in MoSe₂/WSe₂ heterostructures through photoluminescence measurements and vdW‑corrected density functional theory calculations. The photoluminescence of interlayer excitons is strongest at 0° and 60° twist angles and disappears at intermediate angles, a trend corroborated by DFT calculations that reveal enhanced interlayer coupling and band‑edge hybridization at coherent angles, which weakens with increased interlayer separation or when a hexagonal boron nitride monolayer is inserted.
Interlayer excitons were observed at the heterojunctions in van der Waals heterostructures (vdW HSs). However, it is not known how the excitonic phenomena are affected by the stacking order. Here, we report twist-angle-dependent interlayer excitons in MoSe2/WSe2 vdW HSs based on photoluminescence (PL) and vdW-corrected density functional theory calculations. The PL intensity of the interlayer excitons depends primarily on the twist angle: It is enhanced at coherently stacked angles of 0° and 60° (owing to strong interlayer coupling) but disappears at incoherent intermediate angles. The calculations confirm twist-angle-dependent interlayer coupling: The states at the edges of the valence band exhibit a long tail that stretches over the other layer for coherently stacked angles; however, the states are largely confined in the respective layers for intermediate angles. This interlayer hybridization of the band edge states also correlates with the interlayer separation between MoSe2 and WSe2 layers. Furthermore, the interlayer coupling becomes insignificant, irrespective of twist angles, by the incorporation of a hexagonal boron nitride monolayer between MoSe2 and WSe2.
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