Nanoscatterer-Assisted Fluorescence Amplification Technique

Weak fluorescence signals, which are important in research and applications, are often masked by the background. Different amplification techniques are actively investigated. Here, a broadband, geometry-independent and flexible feedback scheme based on the random scattering of dielectric nanoparticl...

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Main Authors: Sylvain Bonnefond, Antoine Reynaud, Julie Cazareth, Sophie Abélanet, Massimo Vassalli, Frédéric Brau, Gian Luca Lippi
Format: Article
Language:English
Published: MDPI AG 2023-10-01
Series:Nanomaterials
Subjects:
Online Access:https://www.mdpi.com/2079-4991/13/21/2875
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author Sylvain Bonnefond
Antoine Reynaud
Julie Cazareth
Sophie Abélanet
Massimo Vassalli
Frédéric Brau
Gian Luca Lippi
author_facet Sylvain Bonnefond
Antoine Reynaud
Julie Cazareth
Sophie Abélanet
Massimo Vassalli
Frédéric Brau
Gian Luca Lippi
author_sort Sylvain Bonnefond
collection DOAJ
description Weak fluorescence signals, which are important in research and applications, are often masked by the background. Different amplification techniques are actively investigated. Here, a broadband, geometry-independent and flexible feedback scheme based on the random scattering of dielectric nanoparticles allows the amplification of a fluorescence signal by partial trapping of the radiation within the sample volume. Amplification of up to a factor of 40 is experimentally demonstrated in ultrapure water with dispersed TiO<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mrow></mrow><mn>2</mn></msub></semantics></math></inline-formula> nanoparticles (30 to 50 nm in diameter) and fluorescein dye at 200 <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi mathvariant="sans-serif">μ</mi></semantics></math></inline-formula>mol concentration (pumped with 5 ns long, 3 mJ laser pulses at 490 nm). The measurements show a measurable reduction in linewidth at the emission peak, indicating that feedback-induced stimulated emission contributes to the large gain observed.
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spelling doaj.art-97436fb909d645caa17d4a122cc2cf502023-11-10T15:09:15ZengMDPI AGNanomaterials2079-49912023-10-011321287510.3390/nano13212875Nanoscatterer-Assisted Fluorescence Amplification TechniqueSylvain Bonnefond0Antoine Reynaud1Julie Cazareth2Sophie Abélanet3Massimo Vassalli4Frédéric Brau5Gian Luca Lippi6Université Côte d’Azur, UMR 7010 CNRS, Institut de Physique de Nice, 06560 Valbonne, FranceUniversité Côte d’Azur, UMR 7275 CNRS, Institut de Pharmacologie Moléculaire et Cellulaire, 06560 Valbonne, FranceUniversité Côte d’Azur, UMR 7275 CNRS, Institut de Pharmacologie Moléculaire et Cellulaire, 06560 Valbonne, FranceUniversité Côte d’Azur, UMR 7275 CNRS, Institut de Pharmacologie Moléculaire et Cellulaire, 06560 Valbonne, FranceJames Watt School of Engineering, University of Glasgow, Glasgow G12 8LT, UKUniversité Côte d’Azur, UMR 7275 CNRS, Institut de Pharmacologie Moléculaire et Cellulaire, 06560 Valbonne, FranceUniversité Côte d’Azur, UMR 7010 CNRS, Institut de Physique de Nice, 06560 Valbonne, FranceWeak fluorescence signals, which are important in research and applications, are often masked by the background. Different amplification techniques are actively investigated. Here, a broadband, geometry-independent and flexible feedback scheme based on the random scattering of dielectric nanoparticles allows the amplification of a fluorescence signal by partial trapping of the radiation within the sample volume. Amplification of up to a factor of 40 is experimentally demonstrated in ultrapure water with dispersed TiO<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mrow></mrow><mn>2</mn></msub></semantics></math></inline-formula> nanoparticles (30 to 50 nm in diameter) and fluorescein dye at 200 <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi mathvariant="sans-serif">μ</mi></semantics></math></inline-formula>mol concentration (pumped with 5 ns long, 3 mJ laser pulses at 490 nm). The measurements show a measurable reduction in linewidth at the emission peak, indicating that feedback-induced stimulated emission contributes to the large gain observed.https://www.mdpi.com/2079-4991/13/21/2875nanoparticlesmultiple scatteringlight amplificationoptical gainlinewidth narrowingstimulated emission
spellingShingle Sylvain Bonnefond
Antoine Reynaud
Julie Cazareth
Sophie Abélanet
Massimo Vassalli
Frédéric Brau
Gian Luca Lippi
Nanoscatterer-Assisted Fluorescence Amplification Technique
Nanomaterials
nanoparticles
multiple scattering
light amplification
optical gain
linewidth narrowing
stimulated emission
title Nanoscatterer-Assisted Fluorescence Amplification Technique
title_full Nanoscatterer-Assisted Fluorescence Amplification Technique
title_fullStr Nanoscatterer-Assisted Fluorescence Amplification Technique
title_full_unstemmed Nanoscatterer-Assisted Fluorescence Amplification Technique
title_short Nanoscatterer-Assisted Fluorescence Amplification Technique
title_sort nanoscatterer assisted fluorescence amplification technique
topic nanoparticles
multiple scattering
light amplification
optical gain
linewidth narrowing
stimulated emission
url https://www.mdpi.com/2079-4991/13/21/2875
work_keys_str_mv AT sylvainbonnefond nanoscattererassistedfluorescenceamplificationtechnique
AT antoinereynaud nanoscattererassistedfluorescenceamplificationtechnique
AT juliecazareth nanoscattererassistedfluorescenceamplificationtechnique
AT sophieabelanet nanoscattererassistedfluorescenceamplificationtechnique
AT massimovassalli nanoscattererassistedfluorescenceamplificationtechnique
AT fredericbrau nanoscattererassistedfluorescenceamplificationtechnique
AT gianlucalippi nanoscattererassistedfluorescenceamplificationtechnique