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Effects of Pump Photon Energy on Generation and Ultrafast Relaxation of Excitons and Charge Carriers in CdSe Nanoplatelets

[Image: see text] We studied the initial nature and relaxation of photoexcited electronic states in CdSe nanoplatelets (NPLs). Ultrafast transient optical absorption (TA) measurements were combined with the theoretical analysis of the formation and decay of excitons, biexcitons, free charge carriers...

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Autores principales: Failla, Michele, García Flórez, Fransisco, Salzmann, Bastiaan B. V., Vanmaekelbergh, Daniel, Stoof, Henk T. C., Siebbeles, Laurens D. A.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2023
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9900632/
https://www.ncbi.nlm.nih.gov/pubmed/36761230
http://dx.doi.org/10.1021/acs.jpcc.2c07292
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author Failla, Michele
García Flórez, Fransisco
Salzmann, Bastiaan B. V.
Vanmaekelbergh, Daniel
Stoof, Henk T. C.
Siebbeles, Laurens D. A.
author_facet Failla, Michele
García Flórez, Fransisco
Salzmann, Bastiaan B. V.
Vanmaekelbergh, Daniel
Stoof, Henk T. C.
Siebbeles, Laurens D. A.
author_sort Failla, Michele
collection PubMed
description [Image: see text] We studied the initial nature and relaxation of photoexcited electronic states in CdSe nanoplatelets (NPLs). Ultrafast transient optical absorption (TA) measurements were combined with the theoretical analysis of the formation and decay of excitons, biexcitons, free charge carriers, and trions. In the latter, photons and excitons were treated as bosons and free charge carriers as fermions. The initial quantum yields of heavy-hole (HH) excitons, light-hole (LH) excitons, and charge carriers vary strongly with photon energy, while thermal relaxation occurs always within 1 ps. After that, the population of LH excitons is negligible due to relaxation to HH excitons or decay into free electrons and holes. Up to the highest average number of about four absorbed photons per NPL in our experiments, we found no signatures of the presence of biexcitons or larger complexes. Biexcitons were only observed due to the interaction of a probe-generated exciton with an exciton produced previously by the pump pulse. For higher pump photon energies, the initial presence of more free charge carriers leads to formation of trions by probe photons. On increasing the number of absorbed pump photons in an NPL, the yield of excitons becomes higher as compared to free charge carriers, since electron–hole recombination becomes more likely. In addition to a TA absorption feature at energy below the HH exciton peak, we also observed a TA signal at the high-energy side of this peak, which we attribute to formation of LH-HH biexcitons or trions consisting of a charge and LH exciton.
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spelling pubmed-99006322023-02-07 Effects of Pump Photon Energy on Generation and Ultrafast Relaxation of Excitons and Charge Carriers in CdSe Nanoplatelets Failla, Michele García Flórez, Fransisco Salzmann, Bastiaan B. V. Vanmaekelbergh, Daniel Stoof, Henk T. C. Siebbeles, Laurens D. A. J Phys Chem C Nanomater Interfaces [Image: see text] We studied the initial nature and relaxation of photoexcited electronic states in CdSe nanoplatelets (NPLs). Ultrafast transient optical absorption (TA) measurements were combined with the theoretical analysis of the formation and decay of excitons, biexcitons, free charge carriers, and trions. In the latter, photons and excitons were treated as bosons and free charge carriers as fermions. The initial quantum yields of heavy-hole (HH) excitons, light-hole (LH) excitons, and charge carriers vary strongly with photon energy, while thermal relaxation occurs always within 1 ps. After that, the population of LH excitons is negligible due to relaxation to HH excitons or decay into free electrons and holes. Up to the highest average number of about four absorbed photons per NPL in our experiments, we found no signatures of the presence of biexcitons or larger complexes. Biexcitons were only observed due to the interaction of a probe-generated exciton with an exciton produced previously by the pump pulse. For higher pump photon energies, the initial presence of more free charge carriers leads to formation of trions by probe photons. On increasing the number of absorbed pump photons in an NPL, the yield of excitons becomes higher as compared to free charge carriers, since electron–hole recombination becomes more likely. In addition to a TA absorption feature at energy below the HH exciton peak, we also observed a TA signal at the high-energy side of this peak, which we attribute to formation of LH-HH biexcitons or trions consisting of a charge and LH exciton. American Chemical Society 2023-01-19 /pmc/articles/PMC9900632/ /pubmed/36761230 http://dx.doi.org/10.1021/acs.jpcc.2c07292 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 Failla, Michele
García Flórez, Fransisco
Salzmann, Bastiaan B. V.
Vanmaekelbergh, Daniel
Stoof, Henk T. C.
Siebbeles, Laurens D. A.
Effects of Pump Photon Energy on Generation and Ultrafast Relaxation of Excitons and Charge Carriers in CdSe Nanoplatelets
title Effects of Pump Photon Energy on Generation and Ultrafast Relaxation of Excitons and Charge Carriers in CdSe Nanoplatelets
title_full Effects of Pump Photon Energy on Generation and Ultrafast Relaxation of Excitons and Charge Carriers in CdSe Nanoplatelets
title_fullStr Effects of Pump Photon Energy on Generation and Ultrafast Relaxation of Excitons and Charge Carriers in CdSe Nanoplatelets
title_full_unstemmed Effects of Pump Photon Energy on Generation and Ultrafast Relaxation of Excitons and Charge Carriers in CdSe Nanoplatelets
title_short Effects of Pump Photon Energy on Generation and Ultrafast Relaxation of Excitons and Charge Carriers in CdSe Nanoplatelets
title_sort effects of pump photon energy on generation and ultrafast relaxation of excitons and charge carriers in cdse nanoplatelets
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9900632/
https://www.ncbi.nlm.nih.gov/pubmed/36761230
http://dx.doi.org/10.1021/acs.jpcc.2c07292
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