2021
DOI: 10.1021/acsanm.1c00889
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Plasmon–Exciton Interactions in Nanometer-Thick Gold-WSe2 Multilayer Structures: Implications for Photodetectors, Sensors, and Light-Emitting Devices

Abstract: Van der Waals materials such as thin films of transition-metal dichalcogenides (TMDCs) manifest strongly bound exciton states in the visible spectrum at ambient conditions that provide an ideal platform for exciton−photon couplings. Utilizing nanometer-thick semiconducting TMDCs in the form of multilayer structures combined with metals can increase significantly the light−matter interaction. In this way, the interaction between excitons and surface-plasmon polaritons emerges as a platform for transferring the… Show more

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Cited by 10 publications
(7 citation statements)
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“…Heterojunctions of metals and semiconducting transition metal dichalcogenides (TMDs) allow various possibilities for the manipulation and exploitation of light–matter interactions, such as the control of plasmonic excitations and plasmon-induced charge injection, transistors, and photovoltaics . Due to their layered structure, excited electrons and holes in TMDs exhibit enhanced Coulomb interactions in both monolayer and bulk (>5 layers) forms, leading to room-temperature stable excitons, which dominate the optical and charge transport properties in these materials.…”
Section: Introductionmentioning
confidence: 99%
“…Heterojunctions of metals and semiconducting transition metal dichalcogenides (TMDs) allow various possibilities for the manipulation and exploitation of light–matter interactions, such as the control of plasmonic excitations and plasmon-induced charge injection, transistors, and photovoltaics . Due to their layered structure, excited electrons and holes in TMDs exhibit enhanced Coulomb interactions in both monolayer and bulk (>5 layers) forms, leading to room-temperature stable excitons, which dominate the optical and charge transport properties in these materials.…”
Section: Introductionmentioning
confidence: 99%
“…A vector-potential approach is used to calculate the radiation from a moving electron in thin films, e.g. to capture the momentum-resolved electron energy-loss spectroscopy (MREELS) [29][30][31]. The current density of a moving electron with the speed of v el along the z-axis is given by J z (⃗ r, t) = −ev el δ (x) δ (y) δ (z − v el t).…”
Section: Non-recoil Approximationmentioning
confidence: 99%
“…In this context, heterojunctions of metals and dielectric materials allow a lot of possibilities for the manipulation and exploitation of light-matter interactions, including ultrafast hot electrons dynamics, magnetooptical effects and nonlinear optical processes 18,[29][30][31][32][33][34][35][36][37][38] . In particular, if the dielectric material is replaced by a semiconducting transition metal dichalcogenide (TMD), we can further boost the control of nanoscale optical excitations [39][40][41][42] , including plasmonic-induced charge injection [43][44][45][46][47][48] , as well as enhance charge dynamics in transistors 49 and photovoltaic devices 50 . Excited electrons and holes in TMDs exhibit enhanced Coulomb interactions in both monolayer and bulk (> 5 layers) forms 51 , leading to room-temperature stable excitons, which dominate the optical and charge transport properties in these materials.…”
Section: Introductionmentioning
confidence: 99%