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Abstract
Monolayer transition-metal dichalcogenide (TMD) materials have attracted a great attention because of their unique properties and promising applications in integrated optoelectronic devices. Being layered materials, they can be stacked vertically to fabricate artificial van der Waals lattices, which offer unique opportunities to tailor the electronic and optical properties. The integration of TMD heterostructures in planar microcavities working in strong coupling regime is particularly important to control the light-matter interactions and form robust polaritons, highly sought for room temperature applications. Here, we demonstrate the systematic control of the coupling-strength by embedding multiple WS2 monolayers in a planar microcavity. The vacuum Rabi splitting is enhanced from 36 meV for one monolayer up to 72 meV for the four-monolayer microcavity. In addition, carrying out time-resolved pump-probe experiments at room temperature we demonstrate the nature of polariton interactions which are dominated by phase space filling effects. Furthermore, we also observe the presence of long-living dark excitations in the multiple monolayer superlattices. Our results pave the way for the realization of polaritonic devices based on planar microcavities embedding multiple monolayers and could potentially lead the way for future devices towards the exploitation of interaction-driven phenomena at room temperature.
The authors embed a multiple quantum-well WS2 heterostructure in a planar microcavity and show the systematic control of the normal mode coupling-strength. They find a strong enhancement of the characteristic time scale, which they attribute to long-lived dark excitations emerging in the structure.
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1 Nanyang Technological University, Division of Physics and Applied Physics, School of Physical and Mathematical Sciences, Singapore, Singapore (GRID:grid.59025.3b) (ISNI:0000 0001 2224 0361)
2 Tsinghua University, State Key Laboratory of Low-Dimensional Quantum Physics and Department of Physics, Beijing, P.R. China (GRID:grid.12527.33) (ISNI:0000 0001 0662 3178)
3 Southeast University, School of Physics, Frontiers Science Center for Mobile Information Communication and Security, Nanjing, P.R. China (GRID:grid.263826.b) (ISNI:0000 0004 1761 0489); Purple Mountain Laboratories, Nanjing, P.R. China (GRID:grid.512509.a) (ISNI:0000 0005 0233 4845)
4 CNR NANOTEC Institute of Nanotechnology, Lecce, Italy (GRID:grid.494551.8) (ISNI:0000 0004 6477 0549); INFN National Institute of Nuclear Physics, Lecce, Italy (GRID:grid.494551.8)
5 Nanyang Technological University, Division of Physics and Applied Physics, School of Physical and Mathematical Sciences, Singapore, Singapore (GRID:grid.59025.3b) (ISNI:0000 0001 2224 0361); Nanyang Technological University, MajuLab, International Joint Research Unit UMI 3654, CNRS, Université Côte d’Azur, Sorbonne Université, National University of Singapore, Singapore, Singapore (GRID:grid.59025.3b) (ISNI:0000 0001 2224 0361)
6 Tsinghua University, State Key Laboratory of Low-Dimensional Quantum Physics and Department of Physics, Beijing, P.R. China (GRID:grid.12527.33) (ISNI:0000 0001 0662 3178); Frontier Science Center for Quantum Information, Beijing, P.R. China (GRID:grid.12527.33) (ISNI:0000 0001 0662 3178); Beijing Academy of Quantum Information Sciences, Beijing, P.R. China (GRID:grid.510904.9) (ISNI:0000 0004 9362 2406); Collaborative Innovation Center of Quantum Matter, Beijing, P.R. China (GRID:grid.495569.2)