Cargando…

Plasmonic enhancement and polarization dependence of nonlinear upconversion emissions from single gold nanorod@SiO(2)@CaF(2):Yb(3+),Er(3+) hybrid core–shell–satellite nanostructures

Lanthanide-doped upconversion nanocrystals (UCNCs) have recently become an attractive nonlinear fluorescence material for use in bioimaging because of their tunable spectral characteristics and exceptional photostability. Plasmonic materials are often introduced into the vicinity of UCNCs to increas...

Descripción completa

Detalles Bibliográficos
Autores principales: He, Jijun, Zheng, Wei, Ligmajer, Filip, Chan, Chi-Fai, Bao, Zhiyong, Wong, Ka-Leung, Chen, Xueyuan, Hao, Jianhua, Dai, Jiyan, Yu, Siu-Fung, Lei, Dang Yuan
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group 2017
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6062198/
https://www.ncbi.nlm.nih.gov/pubmed/30167245
http://dx.doi.org/10.1038/lsa.2016.217
_version_ 1783342354567004160
author He, Jijun
Zheng, Wei
Ligmajer, Filip
Chan, Chi-Fai
Bao, Zhiyong
Wong, Ka-Leung
Chen, Xueyuan
Hao, Jianhua
Dai, Jiyan
Yu, Siu-Fung
Lei, Dang Yuan
author_facet He, Jijun
Zheng, Wei
Ligmajer, Filip
Chan, Chi-Fai
Bao, Zhiyong
Wong, Ka-Leung
Chen, Xueyuan
Hao, Jianhua
Dai, Jiyan
Yu, Siu-Fung
Lei, Dang Yuan
author_sort He, Jijun
collection PubMed
description Lanthanide-doped upconversion nanocrystals (UCNCs) have recently become an attractive nonlinear fluorescence material for use in bioimaging because of their tunable spectral characteristics and exceptional photostability. Plasmonic materials are often introduced into the vicinity of UCNCs to increase their emission intensity by means of enlarging the absorption cross-section and accelerating the radiative decay rate. Moreover, plasmonic nanostructures (e.g., gold nanorods, GNRs) can also influence the polarization state of the UC fluorescence—an effect that is of fundamental importance for fluorescence polarization-based imaging methods yet has not been discussed previously. To study this effect, we synthesized GNR@SiO(2)@CaF(2):Yb(3+),Er(3+) hybrid core–shell–satellite nanostructures with precise control over the thickness of the SiO(2) shell. We evaluated the shell thickness-dependent plasmonic enhancement of the emission intensity in ensemble and studied the plasmonic modulation of the emission polarization at the single-particle level. The hybrid plasmonic UC nanostructures with an optimal shell thickness exhibit an improved bioimaging performance compared with bare UCNCs, and we observed a polarized nature of the light at both UC emission bands, which stems from the relationship between the excitation polarization and GNR orientation. We used electrodynamic simulations combined with Förster resonance energy transfer theory to fully explain the observed effect. Our results provide extensive insights into how the coherent interaction between the emission dipoles of UCNCs and the plasmonic dipoles of the GNR determines the emission polarization state in various situations and thus open the way to the accurate control of the UC emission anisotropy for a wide range of bioimaging and biosensing applications.
format Online
Article
Text
id pubmed-6062198
institution National Center for Biotechnology Information
language English
publishDate 2017
publisher Nature Publishing Group
record_format MEDLINE/PubMed
spelling pubmed-60621982018-08-30 Plasmonic enhancement and polarization dependence of nonlinear upconversion emissions from single gold nanorod@SiO(2)@CaF(2):Yb(3+),Er(3+) hybrid core–shell–satellite nanostructures He, Jijun Zheng, Wei Ligmajer, Filip Chan, Chi-Fai Bao, Zhiyong Wong, Ka-Leung Chen, Xueyuan Hao, Jianhua Dai, Jiyan Yu, Siu-Fung Lei, Dang Yuan Light Sci Appl Original Article Lanthanide-doped upconversion nanocrystals (UCNCs) have recently become an attractive nonlinear fluorescence material for use in bioimaging because of their tunable spectral characteristics and exceptional photostability. Plasmonic materials are often introduced into the vicinity of UCNCs to increase their emission intensity by means of enlarging the absorption cross-section and accelerating the radiative decay rate. Moreover, plasmonic nanostructures (e.g., gold nanorods, GNRs) can also influence the polarization state of the UC fluorescence—an effect that is of fundamental importance for fluorescence polarization-based imaging methods yet has not been discussed previously. To study this effect, we synthesized GNR@SiO(2)@CaF(2):Yb(3+),Er(3+) hybrid core–shell–satellite nanostructures with precise control over the thickness of the SiO(2) shell. We evaluated the shell thickness-dependent plasmonic enhancement of the emission intensity in ensemble and studied the plasmonic modulation of the emission polarization at the single-particle level. The hybrid plasmonic UC nanostructures with an optimal shell thickness exhibit an improved bioimaging performance compared with bare UCNCs, and we observed a polarized nature of the light at both UC emission bands, which stems from the relationship between the excitation polarization and GNR orientation. We used electrodynamic simulations combined with Förster resonance energy transfer theory to fully explain the observed effect. Our results provide extensive insights into how the coherent interaction between the emission dipoles of UCNCs and the plasmonic dipoles of the GNR determines the emission polarization state in various situations and thus open the way to the accurate control of the UC emission anisotropy for a wide range of bioimaging and biosensing applications. Nature Publishing Group 2017-05-19 /pmc/articles/PMC6062198/ /pubmed/30167245 http://dx.doi.org/10.1038/lsa.2016.217 Text en Copyright © 2017 The Author(s) http://creativecommons.org/licenses/by-nc-sa/4.0/ This work is licensed under a Creative Commons Attribution-NonCommercial-ShareAlike 4.0 International License. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in the credit line; if the material is not included under the Creative Commons license, users will need to obtain permission from the license holder to reproduce the material. To view a copy of this license, visit http://creativecommons.org/licenses/by-nc-sa/4.0/
spellingShingle Original Article
He, Jijun
Zheng, Wei
Ligmajer, Filip
Chan, Chi-Fai
Bao, Zhiyong
Wong, Ka-Leung
Chen, Xueyuan
Hao, Jianhua
Dai, Jiyan
Yu, Siu-Fung
Lei, Dang Yuan
Plasmonic enhancement and polarization dependence of nonlinear upconversion emissions from single gold nanorod@SiO(2)@CaF(2):Yb(3+),Er(3+) hybrid core–shell–satellite nanostructures
title Plasmonic enhancement and polarization dependence of nonlinear upconversion emissions from single gold nanorod@SiO(2)@CaF(2):Yb(3+),Er(3+) hybrid core–shell–satellite nanostructures
title_full Plasmonic enhancement and polarization dependence of nonlinear upconversion emissions from single gold nanorod@SiO(2)@CaF(2):Yb(3+),Er(3+) hybrid core–shell–satellite nanostructures
title_fullStr Plasmonic enhancement and polarization dependence of nonlinear upconversion emissions from single gold nanorod@SiO(2)@CaF(2):Yb(3+),Er(3+) hybrid core–shell–satellite nanostructures
title_full_unstemmed Plasmonic enhancement and polarization dependence of nonlinear upconversion emissions from single gold nanorod@SiO(2)@CaF(2):Yb(3+),Er(3+) hybrid core–shell–satellite nanostructures
title_short Plasmonic enhancement and polarization dependence of nonlinear upconversion emissions from single gold nanorod@SiO(2)@CaF(2):Yb(3+),Er(3+) hybrid core–shell–satellite nanostructures
title_sort plasmonic enhancement and polarization dependence of nonlinear upconversion emissions from single gold nanorod@sio(2)@caf(2):yb(3+),er(3+) hybrid core–shell–satellite nanostructures
topic Original Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6062198/
https://www.ncbi.nlm.nih.gov/pubmed/30167245
http://dx.doi.org/10.1038/lsa.2016.217
work_keys_str_mv AT hejijun plasmonicenhancementandpolarizationdependenceofnonlinearupconversionemissionsfromsinglegoldnanorodsio2caf2yb3er3hybridcoreshellsatellitenanostructures
AT zhengwei plasmonicenhancementandpolarizationdependenceofnonlinearupconversionemissionsfromsinglegoldnanorodsio2caf2yb3er3hybridcoreshellsatellitenanostructures
AT ligmajerfilip plasmonicenhancementandpolarizationdependenceofnonlinearupconversionemissionsfromsinglegoldnanorodsio2caf2yb3er3hybridcoreshellsatellitenanostructures
AT chanchifai plasmonicenhancementandpolarizationdependenceofnonlinearupconversionemissionsfromsinglegoldnanorodsio2caf2yb3er3hybridcoreshellsatellitenanostructures
AT baozhiyong plasmonicenhancementandpolarizationdependenceofnonlinearupconversionemissionsfromsinglegoldnanorodsio2caf2yb3er3hybridcoreshellsatellitenanostructures
AT wongkaleung plasmonicenhancementandpolarizationdependenceofnonlinearupconversionemissionsfromsinglegoldnanorodsio2caf2yb3er3hybridcoreshellsatellitenanostructures
AT chenxueyuan plasmonicenhancementandpolarizationdependenceofnonlinearupconversionemissionsfromsinglegoldnanorodsio2caf2yb3er3hybridcoreshellsatellitenanostructures
AT haojianhua plasmonicenhancementandpolarizationdependenceofnonlinearupconversionemissionsfromsinglegoldnanorodsio2caf2yb3er3hybridcoreshellsatellitenanostructures
AT daijiyan plasmonicenhancementandpolarizationdependenceofnonlinearupconversionemissionsfromsinglegoldnanorodsio2caf2yb3er3hybridcoreshellsatellitenanostructures
AT yusiufung plasmonicenhancementandpolarizationdependenceofnonlinearupconversionemissionsfromsinglegoldnanorodsio2caf2yb3er3hybridcoreshellsatellitenanostructures
AT leidangyuan plasmonicenhancementandpolarizationdependenceofnonlinearupconversionemissionsfromsinglegoldnanorodsio2caf2yb3er3hybridcoreshellsatellitenanostructures