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Filling Exciton Trap-States in Two-Dimensional Tungsten Disulfide (WS(2)) and Diselenide (WSe(2)) Monolayers

Two-dimensional transition metal dichalcogenides (2D-TMDs) hold a great potential to platform future flexible optoelectronics. The beating hearts of these materials are their excitons known as X(A) and X(B), which arise from transitions between spin-orbit split (SOS) levels in the conduction and val...

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Autores principales: Ezgi Eroglu, Zeynep, Contreras, Dillon, Bahrami, Pouya, Azam, Nurul, Mahjouri-Samani, Masoud, Boulesbaa, Abdelaziz
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2021
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8002918/
https://www.ncbi.nlm.nih.gov/pubmed/33803656
http://dx.doi.org/10.3390/nano11030770
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author Ezgi Eroglu, Zeynep
Contreras, Dillon
Bahrami, Pouya
Azam, Nurul
Mahjouri-Samani, Masoud
Boulesbaa, Abdelaziz
author_facet Ezgi Eroglu, Zeynep
Contreras, Dillon
Bahrami, Pouya
Azam, Nurul
Mahjouri-Samani, Masoud
Boulesbaa, Abdelaziz
author_sort Ezgi Eroglu, Zeynep
collection PubMed
description Two-dimensional transition metal dichalcogenides (2D-TMDs) hold a great potential to platform future flexible optoelectronics. The beating hearts of these materials are their excitons known as X(A) and X(B), which arise from transitions between spin-orbit split (SOS) levels in the conduction and valence bands at the K-point. The functionality of 2D-TMD-based devices is determined by the dynamics of these excitons. One of the most consequential channels of exciton decay on the device functionality is the defect-assisted recombination (DAR). Here, we employ steady-state absorption and emission spectroscopies, and pump density-dependent femtosecond transient absorption spectroscopy to report on the effect of DAR on the lifetime of excitons in monolayers of tungsten disulfide (2D-WS(2)) and diselenide (2D-WSe(2)). These pump-probe measurements suggested that while exciton decay dynamics in both monolayers are driven by DAR, in 2D-WS(2), defect states near the X(B) exciton fill up before those near the X(A) exciton. However, in the 2D-WSe(2) monolayer, the defect states fill up similarly. Understanding the contribution of DAR on the lifetime of excitons and the partition of this decay channel between X(A) and X(B) excitons may open new horizons for the incorporation of 2D-TMD materials in future optoelectronics.
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spelling pubmed-80029182021-03-28 Filling Exciton Trap-States in Two-Dimensional Tungsten Disulfide (WS(2)) and Diselenide (WSe(2)) Monolayers Ezgi Eroglu, Zeynep Contreras, Dillon Bahrami, Pouya Azam, Nurul Mahjouri-Samani, Masoud Boulesbaa, Abdelaziz Nanomaterials (Basel) Article Two-dimensional transition metal dichalcogenides (2D-TMDs) hold a great potential to platform future flexible optoelectronics. The beating hearts of these materials are their excitons known as X(A) and X(B), which arise from transitions between spin-orbit split (SOS) levels in the conduction and valence bands at the K-point. The functionality of 2D-TMD-based devices is determined by the dynamics of these excitons. One of the most consequential channels of exciton decay on the device functionality is the defect-assisted recombination (DAR). Here, we employ steady-state absorption and emission spectroscopies, and pump density-dependent femtosecond transient absorption spectroscopy to report on the effect of DAR on the lifetime of excitons in monolayers of tungsten disulfide (2D-WS(2)) and diselenide (2D-WSe(2)). These pump-probe measurements suggested that while exciton decay dynamics in both monolayers are driven by DAR, in 2D-WS(2), defect states near the X(B) exciton fill up before those near the X(A) exciton. However, in the 2D-WSe(2) monolayer, the defect states fill up similarly. Understanding the contribution of DAR on the lifetime of excitons and the partition of this decay channel between X(A) and X(B) excitons may open new horizons for the incorporation of 2D-TMD materials in future optoelectronics. MDPI 2021-03-18 /pmc/articles/PMC8002918/ /pubmed/33803656 http://dx.doi.org/10.3390/nano11030770 Text en © 2021 by the authors. https://creativecommons.org/licenses/by/4.0/Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (http://creativecommons.org/licenses/by/4.0/ (https://creativecommons.org/licenses/by/4.0/) ).
spellingShingle Article
Ezgi Eroglu, Zeynep
Contreras, Dillon
Bahrami, Pouya
Azam, Nurul
Mahjouri-Samani, Masoud
Boulesbaa, Abdelaziz
Filling Exciton Trap-States in Two-Dimensional Tungsten Disulfide (WS(2)) and Diselenide (WSe(2)) Monolayers
title Filling Exciton Trap-States in Two-Dimensional Tungsten Disulfide (WS(2)) and Diselenide (WSe(2)) Monolayers
title_full Filling Exciton Trap-States in Two-Dimensional Tungsten Disulfide (WS(2)) and Diselenide (WSe(2)) Monolayers
title_fullStr Filling Exciton Trap-States in Two-Dimensional Tungsten Disulfide (WS(2)) and Diselenide (WSe(2)) Monolayers
title_full_unstemmed Filling Exciton Trap-States in Two-Dimensional Tungsten Disulfide (WS(2)) and Diselenide (WSe(2)) Monolayers
title_short Filling Exciton Trap-States in Two-Dimensional Tungsten Disulfide (WS(2)) and Diselenide (WSe(2)) Monolayers
title_sort filling exciton trap-states in two-dimensional tungsten disulfide (ws(2)) and diselenide (wse(2)) monolayers
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8002918/
https://www.ncbi.nlm.nih.gov/pubmed/33803656
http://dx.doi.org/10.3390/nano11030770
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