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Colloidal-Quantum-Dot Ring Lasers with Active Color Control
[Image: see text] To improve the photophysical performance of colloidal quantum dots for laser applications, sophisticated core/shell geometries have been developed. Typically, a wider bandgap semiconductor is added as a shell to enhance the gain from the quantum-dot core. This shell is designed to...
Autores principales: | , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
American Chemical Society
2017
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Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5817622/ https://www.ncbi.nlm.nih.gov/pubmed/29283266 http://dx.doi.org/10.1021/acs.nanolett.7b04495 |
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author | le Feber, Boris Prins, Ferry De Leo, Eva Rabouw, Freddy T. Norris, David J. |
author_facet | le Feber, Boris Prins, Ferry De Leo, Eva Rabouw, Freddy T. Norris, David J. |
author_sort | le Feber, Boris |
collection | PubMed |
description | [Image: see text] To improve the photophysical performance of colloidal quantum dots for laser applications, sophisticated core/shell geometries have been developed. Typically, a wider bandgap semiconductor is added as a shell to enhance the gain from the quantum-dot core. This shell is designed to electronically isolate the core, funnel excitons to it, and reduce nonradiative Auger recombination. However, the shell could also potentially provide a secondary source of gain, leading to further versatility in these materials. Here we develop high-quality quantum-dot ring lasers that not only exhibit lasing from both the core and the shell but also the ability to switch between them. We fabricate ring resonators (with quality factors up to ∼2500) consisting only of CdSe/CdS/ZnS core/shell/shell quantum dots using a simple template-stripping process. We then examine lasing as a function of the optical excitation power and ring radius. In resonators with quality factors >1000, excitons in the CdSe cores lead to red lasing with thresholds at ∼25 μJ/cm(2). With increasing power, green lasing from the CdS shell emerges (>100 μJ/cm(2)) and then the red lasing begins to disappear (>250 μJ/cm(2)). We present a rate-equation model that can explain this color switching as a competition between exciton localization into the core and stimulated emission from excitons in the shell. Moreover, by lowering the quality factor of the cavity we can engineer the device to exhibit only green lasing. The mechanism demonstrated here provides a potential route toward color-switchable quantum-dot lasers. |
format | Online Article Text |
id | pubmed-5817622 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2017 |
publisher | American Chemical Society |
record_format | MEDLINE/PubMed |
spelling | pubmed-58176222018-02-20 Colloidal-Quantum-Dot Ring Lasers with Active Color Control le Feber, Boris Prins, Ferry De Leo, Eva Rabouw, Freddy T. Norris, David J. Nano Lett [Image: see text] To improve the photophysical performance of colloidal quantum dots for laser applications, sophisticated core/shell geometries have been developed. Typically, a wider bandgap semiconductor is added as a shell to enhance the gain from the quantum-dot core. This shell is designed to electronically isolate the core, funnel excitons to it, and reduce nonradiative Auger recombination. However, the shell could also potentially provide a secondary source of gain, leading to further versatility in these materials. Here we develop high-quality quantum-dot ring lasers that not only exhibit lasing from both the core and the shell but also the ability to switch between them. We fabricate ring resonators (with quality factors up to ∼2500) consisting only of CdSe/CdS/ZnS core/shell/shell quantum dots using a simple template-stripping process. We then examine lasing as a function of the optical excitation power and ring radius. In resonators with quality factors >1000, excitons in the CdSe cores lead to red lasing with thresholds at ∼25 μJ/cm(2). With increasing power, green lasing from the CdS shell emerges (>100 μJ/cm(2)) and then the red lasing begins to disappear (>250 μJ/cm(2)). We present a rate-equation model that can explain this color switching as a competition between exciton localization into the core and stimulated emission from excitons in the shell. Moreover, by lowering the quality factor of the cavity we can engineer the device to exhibit only green lasing. The mechanism demonstrated here provides a potential route toward color-switchable quantum-dot lasers. American Chemical Society 2017-12-28 2018-02-14 /pmc/articles/PMC5817622/ /pubmed/29283266 http://dx.doi.org/10.1021/acs.nanolett.7b04495 Text en Copyright © 2017 American Chemical Society This is an open access article published under an ACS AuthorChoice License (http://pubs.acs.org/page/policy/authorchoice_termsofuse.html) , which permits copying and redistribution of the article or any adaptations for non-commercial purposes. |
spellingShingle | le Feber, Boris Prins, Ferry De Leo, Eva Rabouw, Freddy T. Norris, David J. Colloidal-Quantum-Dot Ring Lasers with Active Color Control |
title | Colloidal-Quantum-Dot Ring Lasers with Active Color
Control |
title_full | Colloidal-Quantum-Dot Ring Lasers with Active Color
Control |
title_fullStr | Colloidal-Quantum-Dot Ring Lasers with Active Color
Control |
title_full_unstemmed | Colloidal-Quantum-Dot Ring Lasers with Active Color
Control |
title_short | Colloidal-Quantum-Dot Ring Lasers with Active Color
Control |
title_sort | colloidal-quantum-dot ring lasers with active color
control |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5817622/ https://www.ncbi.nlm.nih.gov/pubmed/29283266 http://dx.doi.org/10.1021/acs.nanolett.7b04495 |
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