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Hot Carrier Cooling and Trapping in Atomically Thin WS(2) Probed by Three-Pulse Femtosecond Spectroscopy

[Image: see text] Transition metal dichalcogenides (TMDs) have shown outstanding semiconducting properties which make them promising materials for next-generation optoelectronic and electronic devices. These properties are imparted by fundamental carrier–carrier and carrier–phonon interactions that...

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Autores principales: Wang, Tong, Hopper, Thomas R., Mondal, Navendu, Liu, Sihui, Yao, Chengning, Zheng, Xijia, Torrisi, Felice, Bakulin, Artem A.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2023
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10100566/
https://www.ncbi.nlm.nih.gov/pubmed/36939760
http://dx.doi.org/10.1021/acsnano.2c10479
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author Wang, Tong
Hopper, Thomas R.
Mondal, Navendu
Liu, Sihui
Yao, Chengning
Zheng, Xijia
Torrisi, Felice
Bakulin, Artem A.
author_facet Wang, Tong
Hopper, Thomas R.
Mondal, Navendu
Liu, Sihui
Yao, Chengning
Zheng, Xijia
Torrisi, Felice
Bakulin, Artem A.
author_sort Wang, Tong
collection PubMed
description [Image: see text] Transition metal dichalcogenides (TMDs) have shown outstanding semiconducting properties which make them promising materials for next-generation optoelectronic and electronic devices. These properties are imparted by fundamental carrier–carrier and carrier–phonon interactions that are foundational to hot carrier cooling. Recent transient absorption studies have reported ultrafast time scales for carrier cooling in TMDs that can be slowed at high excitation densities via a hot-phonon bottleneck (HPB) and discussed these findings in the light of optoelectronic applications. However, quantitative descriptions of the HPB in TMDs, including details of the electron–lattice coupling and how cooling is affected by the redistribution of energy between carriers, are still lacking. Here, we use femtosecond pump–push–probe spectroscopy as a single approach to systematically characterize the scattering of hot carriers with optical phonons, cold carriers, and defects in a benchmark TMD monolayer of polycrystalline WS(2). By controlling the interband pump and intraband push excitations, we observe, in real-time (i) an extremely rapid “intrinsic” cooling rate of ∼18 ± 2.7 eV/ps, which can be slowed with increasing hot carrier density, (ii) the deprecation of this HPB at elevated cold carrier densities, exposing a previously undisclosed role of the carrier–carrier interactions in mediating cooling, and (iii) the interception of high energy hot carriers on the subpicosecond time scale by lattice defects, which may account for the lower photoluminescence yield of TMDs when excited above band gap.
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spelling pubmed-101005662023-04-14 Hot Carrier Cooling and Trapping in Atomically Thin WS(2) Probed by Three-Pulse Femtosecond Spectroscopy Wang, Tong Hopper, Thomas R. Mondal, Navendu Liu, Sihui Yao, Chengning Zheng, Xijia Torrisi, Felice Bakulin, Artem A. ACS Nano [Image: see text] Transition metal dichalcogenides (TMDs) have shown outstanding semiconducting properties which make them promising materials for next-generation optoelectronic and electronic devices. These properties are imparted by fundamental carrier–carrier and carrier–phonon interactions that are foundational to hot carrier cooling. Recent transient absorption studies have reported ultrafast time scales for carrier cooling in TMDs that can be slowed at high excitation densities via a hot-phonon bottleneck (HPB) and discussed these findings in the light of optoelectronic applications. However, quantitative descriptions of the HPB in TMDs, including details of the electron–lattice coupling and how cooling is affected by the redistribution of energy between carriers, are still lacking. Here, we use femtosecond pump–push–probe spectroscopy as a single approach to systematically characterize the scattering of hot carriers with optical phonons, cold carriers, and defects in a benchmark TMD monolayer of polycrystalline WS(2). By controlling the interband pump and intraband push excitations, we observe, in real-time (i) an extremely rapid “intrinsic” cooling rate of ∼18 ± 2.7 eV/ps, which can be slowed with increasing hot carrier density, (ii) the deprecation of this HPB at elevated cold carrier densities, exposing a previously undisclosed role of the carrier–carrier interactions in mediating cooling, and (iii) the interception of high energy hot carriers on the subpicosecond time scale by lattice defects, which may account for the lower photoluminescence yield of TMDs when excited above band gap. American Chemical Society 2023-03-20 /pmc/articles/PMC10100566/ /pubmed/36939760 http://dx.doi.org/10.1021/acsnano.2c10479 Text en © 2023 The Authors. Published by American Chemical Society https://creativecommons.org/licenses/by/4.0/Permits the broadest form of re-use including for commercial purposes, provided that author attribution and integrity are maintained (https://creativecommons.org/licenses/by/4.0/).
spellingShingle Wang, Tong
Hopper, Thomas R.
Mondal, Navendu
Liu, Sihui
Yao, Chengning
Zheng, Xijia
Torrisi, Felice
Bakulin, Artem A.
Hot Carrier Cooling and Trapping in Atomically Thin WS(2) Probed by Three-Pulse Femtosecond Spectroscopy
title Hot Carrier Cooling and Trapping in Atomically Thin WS(2) Probed by Three-Pulse Femtosecond Spectroscopy
title_full Hot Carrier Cooling and Trapping in Atomically Thin WS(2) Probed by Three-Pulse Femtosecond Spectroscopy
title_fullStr Hot Carrier Cooling and Trapping in Atomically Thin WS(2) Probed by Three-Pulse Femtosecond Spectroscopy
title_full_unstemmed Hot Carrier Cooling and Trapping in Atomically Thin WS(2) Probed by Three-Pulse Femtosecond Spectroscopy
title_short Hot Carrier Cooling and Trapping in Atomically Thin WS(2) Probed by Three-Pulse Femtosecond Spectroscopy
title_sort hot carrier cooling and trapping in atomically thin ws(2) probed by three-pulse femtosecond spectroscopy
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10100566/
https://www.ncbi.nlm.nih.gov/pubmed/36939760
http://dx.doi.org/10.1021/acsnano.2c10479
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