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Synergy between plasmonic nanocavities and random lasing modes: a tool to dequench plasmon quenched fluorophore emission
Metal nanoparticles (NPs) can be employed to modify the emission level of a dye emitter by tailoring the spectral overlap of the optical gain and localized surface plasmon resonance (LSPR). In the case of plasmonic random lasers, tuning the spectral overlap by manipulating metal NPs changes the scat...
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Published in: | Physical chemistry chemical physics : PCCP 2023-10, Vol.25 (41), p.28336-28349 |
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description | Metal nanoparticles (NPs) can be employed to modify the emission level of a dye emitter by tailoring the spectral overlap of the optical gain and localized surface plasmon resonance (LSPR). In the case of plasmonic random lasers, tuning the spectral overlap by manipulating metal NPs changes the scattering properties of the system, which is crucial in random lasers (RLs). In order to overcome this drawback, the emitter gain spectrum across the LSPR is tuned by appropriately choosing various dye emitters. A system with Au nanoislands (NIs) randomly distributed on the surface of vertically aligned ZnO nanorods on a glass substrate coated with three different dye emitters has been employed to study the metal-gain interaction as a function of spectral overlap. It is observed that the photoluminescence is quenched in the presence of Au NIs for all the three dye emitters; however, the degree of quenching is found to be directly proportional to the extent of spectral overlap of the LSPR and the fluorophore emission spectrum, with the resonantly coupled systems exhibiting higher random lasing thresholds. However, a dequenching of the emission is observed under spectrally off-resonant conditions, leading to a lower threshold RL. The effect of tailoring of the metal-gain interaction on the coherent and incoherent intensity components of RL emission is studied to elucidate the contrasting results of photoluminescence and RL emission. As the optical gain shifts away from the LSPR peak, the RL emission is dominated by the coherent intensity. The speckle-like field distributions of the RL modes couple to the plasmonic nanocavities along with a reduced absorption loss for the off-resonant case, leading to an enhanced stimulated emission. Hence, a synergy between random laser modes, plasmonic nanocavities and optimum spectral overlap has been utilized as a tool to dequench the plasmon quenched fluorophore emission.
Dequenching of the plasmon quenched fluorophore emission
via
the synergy of random lasing modes and spectral overlap optimized plasmonic nanocavities. |
doi_str_mv | 10.1039/d3cp04151d |
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Dequenching of the plasmon quenched fluorophore emission
via
the synergy of random lasing modes and spectral overlap optimized plasmonic nanocavities.</description><identifier>ISSN: 1463-9076</identifier><identifier>EISSN: 1463-9084</identifier><identifier>DOI: 10.1039/d3cp04151d</identifier><language>eng</language><publisher>Cambridge: Royal Society of Chemistry</publisher><subject>Dyes ; Emission analysis ; Emitters ; Glass substrates ; Laser modes ; Lasers ; Lasing ; Nanoparticles ; Nanorods ; Photoluminescence ; Plasmonics ; Quenching ; Spectral emittance ; Stimulated emission ; Surface plasmon resonance ; Zinc oxide</subject><ispartof>Physical chemistry chemical physics : PCCP, 2023-10, Vol.25 (41), p.28336-28349</ispartof><rights>Copyright Royal Society of Chemistry 2023</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><cites>FETCH-LOGICAL-c273t-afd246d5728972e819d12537aaf56c2797397877b6da76360612650c5e2dd8053</cites><orcidid>0000-0002-9608-5867 ; 0000-0003-0442-3599 ; 0000-0002-6979-799X ; 0000-0001-7832-3721 ; 0000-0003-3974-2012 ; 0000-0002-8099-6690 ; 0000-0003-1207-0906 ; 0000-0003-4846-8262</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780,27901,27902</link.rule.ids></links><search><creatorcontrib>Yadav, Renu</creatorcontrib><creatorcontrib>Pal, Sourabh</creatorcontrib><creatorcontrib>Jana, Subhajit</creatorcontrib><creatorcontrib>Roy, Shuvajit</creatorcontrib><creatorcontrib>Debnath, Kapil</creatorcontrib><creatorcontrib>Ray, Samit K</creatorcontrib><creatorcontrib>Brundavanam, Maruthi M</creatorcontrib><creatorcontrib>Bhaktha, Shivakiran</creatorcontrib><title>Synergy between plasmonic nanocavities and random lasing modes: a tool to dequench plasmon quenched fluorophore emission</title><title>Physical chemistry chemical physics : PCCP</title><description>Metal nanoparticles (NPs) can be employed to modify the emission level of a dye emitter by tailoring the spectral overlap of the optical gain and localized surface plasmon resonance (LSPR). In the case of plasmonic random lasers, tuning the spectral overlap by manipulating metal NPs changes the scattering properties of the system, which is crucial in random lasers (RLs). In order to overcome this drawback, the emitter gain spectrum across the LSPR is tuned by appropriately choosing various dye emitters. A system with Au nanoislands (NIs) randomly distributed on the surface of vertically aligned ZnO nanorods on a glass substrate coated with three different dye emitters has been employed to study the metal-gain interaction as a function of spectral overlap. It is observed that the photoluminescence is quenched in the presence of Au NIs for all the three dye emitters; however, the degree of quenching is found to be directly proportional to the extent of spectral overlap of the LSPR and the fluorophore emission spectrum, with the resonantly coupled systems exhibiting higher random lasing thresholds. However, a dequenching of the emission is observed under spectrally off-resonant conditions, leading to a lower threshold RL. The effect of tailoring of the metal-gain interaction on the coherent and incoherent intensity components of RL emission is studied to elucidate the contrasting results of photoluminescence and RL emission. As the optical gain shifts away from the LSPR peak, the RL emission is dominated by the coherent intensity. The speckle-like field distributions of the RL modes couple to the plasmonic nanocavities along with a reduced absorption loss for the off-resonant case, leading to an enhanced stimulated emission. Hence, a synergy between random laser modes, plasmonic nanocavities and optimum spectral overlap has been utilized as a tool to dequench the plasmon quenched fluorophore emission.
Dequenching of the plasmon quenched fluorophore emission
via
the synergy of random lasing modes and spectral overlap optimized plasmonic nanocavities.</description><subject>Dyes</subject><subject>Emission analysis</subject><subject>Emitters</subject><subject>Glass substrates</subject><subject>Laser modes</subject><subject>Lasers</subject><subject>Lasing</subject><subject>Nanoparticles</subject><subject>Nanorods</subject><subject>Photoluminescence</subject><subject>Plasmonics</subject><subject>Quenching</subject><subject>Spectral emittance</subject><subject>Stimulated emission</subject><subject>Surface plasmon resonance</subject><subject>Zinc oxide</subject><issn>1463-9076</issn><issn>1463-9084</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2023</creationdate><recordtype>article</recordtype><recordid>eNpd0UtLAzEUBeBBFKzVjXsh4EaEah6Tx7iT1hcICup6SJM77ZSZZEymav-90WoFNze58HE5cLLskOAzgllxbpnpcE44sVvZgOSCjQqs8u3NX4rdbC_GBcY4ITbIPp5WDsJshabQvwM41DU6tt7VBjntvNFvdV9DRNpZFNLwLUqgdjPUegvxAmnUe9-kgSy8LsGZ-e8JtF7BoqpZ-uC7uQ-AoK1jrL3bz3Yq3UQ4-HmH2cv11fP4dnT_cHM3vrwfGSpZP9KVpbmwXFJVSAqKFJZQzqTWFReJFJIVUkk5FVZLwQQWhAqODQdqrcKcDbOT9d0u-BQo9mUKYKBptAO_jCVVUmEiFReJHv-jC78MLqVLShEuC5bTpE7XygQfY4Cq7ELd6rAqCS6_SignbPz4XcIk4aM1DtFs3F9J7BMDqYQ2</recordid><startdate>20231025</startdate><enddate>20231025</enddate><creator>Yadav, Renu</creator><creator>Pal, Sourabh</creator><creator>Jana, Subhajit</creator><creator>Roy, Shuvajit</creator><creator>Debnath, Kapil</creator><creator>Ray, Samit K</creator><creator>Brundavanam, Maruthi M</creator><creator>Bhaktha, Shivakiran</creator><general>Royal Society of Chemistry</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7SR</scope><scope>7U5</scope><scope>8BQ</scope><scope>8FD</scope><scope>JG9</scope><scope>L7M</scope><scope>7X8</scope><orcidid>https://orcid.org/0000-0002-9608-5867</orcidid><orcidid>https://orcid.org/0000-0003-0442-3599</orcidid><orcidid>https://orcid.org/0000-0002-6979-799X</orcidid><orcidid>https://orcid.org/0000-0001-7832-3721</orcidid><orcidid>https://orcid.org/0000-0003-3974-2012</orcidid><orcidid>https://orcid.org/0000-0002-8099-6690</orcidid><orcidid>https://orcid.org/0000-0003-1207-0906</orcidid><orcidid>https://orcid.org/0000-0003-4846-8262</orcidid></search><sort><creationdate>20231025</creationdate><title>Synergy between plasmonic nanocavities and random lasing modes: a tool to dequench plasmon quenched fluorophore emission</title><author>Yadav, Renu ; Pal, Sourabh ; Jana, Subhajit ; Roy, Shuvajit ; Debnath, Kapil ; Ray, Samit K ; Brundavanam, Maruthi M ; Bhaktha, Shivakiran</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c273t-afd246d5728972e819d12537aaf56c2797397877b6da76360612650c5e2dd8053</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2023</creationdate><topic>Dyes</topic><topic>Emission analysis</topic><topic>Emitters</topic><topic>Glass substrates</topic><topic>Laser modes</topic><topic>Lasers</topic><topic>Lasing</topic><topic>Nanoparticles</topic><topic>Nanorods</topic><topic>Photoluminescence</topic><topic>Plasmonics</topic><topic>Quenching</topic><topic>Spectral emittance</topic><topic>Stimulated emission</topic><topic>Surface plasmon resonance</topic><topic>Zinc oxide</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Yadav, Renu</creatorcontrib><creatorcontrib>Pal, Sourabh</creatorcontrib><creatorcontrib>Jana, Subhajit</creatorcontrib><creatorcontrib>Roy, Shuvajit</creatorcontrib><creatorcontrib>Debnath, Kapil</creatorcontrib><creatorcontrib>Ray, Samit K</creatorcontrib><creatorcontrib>Brundavanam, Maruthi M</creatorcontrib><creatorcontrib>Bhaktha, Shivakiran</creatorcontrib><collection>CrossRef</collection><collection>Engineered Materials Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>MEDLINE - Academic</collection><jtitle>Physical chemistry chemical physics : PCCP</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Yadav, Renu</au><au>Pal, Sourabh</au><au>Jana, Subhajit</au><au>Roy, Shuvajit</au><au>Debnath, Kapil</au><au>Ray, Samit K</au><au>Brundavanam, Maruthi M</au><au>Bhaktha, Shivakiran</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Synergy between plasmonic nanocavities and random lasing modes: a tool to dequench plasmon quenched fluorophore emission</atitle><jtitle>Physical chemistry chemical physics : PCCP</jtitle><date>2023-10-25</date><risdate>2023</risdate><volume>25</volume><issue>41</issue><spage>28336</spage><epage>28349</epage><pages>28336-28349</pages><issn>1463-9076</issn><eissn>1463-9084</eissn><abstract>Metal nanoparticles (NPs) can be employed to modify the emission level of a dye emitter by tailoring the spectral overlap of the optical gain and localized surface plasmon resonance (LSPR). In the case of plasmonic random lasers, tuning the spectral overlap by manipulating metal NPs changes the scattering properties of the system, which is crucial in random lasers (RLs). In order to overcome this drawback, the emitter gain spectrum across the LSPR is tuned by appropriately choosing various dye emitters. A system with Au nanoislands (NIs) randomly distributed on the surface of vertically aligned ZnO nanorods on a glass substrate coated with three different dye emitters has been employed to study the metal-gain interaction as a function of spectral overlap. It is observed that the photoluminescence is quenched in the presence of Au NIs for all the three dye emitters; however, the degree of quenching is found to be directly proportional to the extent of spectral overlap of the LSPR and the fluorophore emission spectrum, with the resonantly coupled systems exhibiting higher random lasing thresholds. However, a dequenching of the emission is observed under spectrally off-resonant conditions, leading to a lower threshold RL. The effect of tailoring of the metal-gain interaction on the coherent and incoherent intensity components of RL emission is studied to elucidate the contrasting results of photoluminescence and RL emission. As the optical gain shifts away from the LSPR peak, the RL emission is dominated by the coherent intensity. The speckle-like field distributions of the RL modes couple to the plasmonic nanocavities along with a reduced absorption loss for the off-resonant case, leading to an enhanced stimulated emission. Hence, a synergy between random laser modes, plasmonic nanocavities and optimum spectral overlap has been utilized as a tool to dequench the plasmon quenched fluorophore emission.
Dequenching of the plasmon quenched fluorophore emission
via
the synergy of random lasing modes and spectral overlap optimized plasmonic nanocavities.</abstract><cop>Cambridge</cop><pub>Royal Society of Chemistry</pub><doi>10.1039/d3cp04151d</doi><tpages>14</tpages><orcidid>https://orcid.org/0000-0002-9608-5867</orcidid><orcidid>https://orcid.org/0000-0003-0442-3599</orcidid><orcidid>https://orcid.org/0000-0002-6979-799X</orcidid><orcidid>https://orcid.org/0000-0001-7832-3721</orcidid><orcidid>https://orcid.org/0000-0003-3974-2012</orcidid><orcidid>https://orcid.org/0000-0002-8099-6690</orcidid><orcidid>https://orcid.org/0000-0003-1207-0906</orcidid><orcidid>https://orcid.org/0000-0003-4846-8262</orcidid></addata></record> |
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subjects | Dyes Emission analysis Emitters Glass substrates Laser modes Lasers Lasing Nanoparticles Nanorods Photoluminescence Plasmonics Quenching Spectral emittance Stimulated emission Surface plasmon resonance Zinc oxide |
title | Synergy between plasmonic nanocavities and random lasing modes: a tool to dequench plasmon quenched fluorophore emission |
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