Effect of the excitation setup in the improved enhancement factor of covered-gold-nanorod-dimer antennas

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Devices possessing the ability to sense both electrically and optically molecular targets are of fundamental and technological interest. Towards this end, it has been shown that covering the ends of gapped gold-nanorod-dimer nanoantennas can improve the enhancement factor (EF) that quantifies the na...

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Detalles Bibliográficos
Autores: Ramos, Iván A., León Hilario, L. M., Pedano, María L., Reynoso, Andrés A.
Formato: artículo
Fecha de Publicación:2022
Institución:Universidad Nacional de Ingeniería
Repositorio:UNI-Tesis
Lenguaje:inglés
OAI Identifier:oai:cybertesis.uni.edu.pe:20.500.14076/29110
Enlace del recurso:http://hdl.handle.net/20.500.14076/29110
https://doi.org/10.1039/D2CP03124H
Nivel de acceso:acceso abierto
Materia:Nanoantenna efficiency
Enhancement factor (EF)
Surface-enhancement Raman spectroscopy (SERS)
Antennas
https://purl.org/pe-repo/ocde/ford#2.10.00
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dc.title.en.fl_str_mv Effect of the excitation setup in the improved enhancement factor of covered-gold-nanorod-dimer antennas
title Effect of the excitation setup in the improved enhancement factor of covered-gold-nanorod-dimer antennas
spellingShingle Effect of the excitation setup in the improved enhancement factor of covered-gold-nanorod-dimer antennas
Ramos, Iván A.
Nanoantenna efficiency
Enhancement factor (EF)
Surface-enhancement Raman spectroscopy (SERS)
Antennas
https://purl.org/pe-repo/ocde/ford#2.10.00
title_short Effect of the excitation setup in the improved enhancement factor of covered-gold-nanorod-dimer antennas
title_full Effect of the excitation setup in the improved enhancement factor of covered-gold-nanorod-dimer antennas
title_fullStr Effect of the excitation setup in the improved enhancement factor of covered-gold-nanorod-dimer antennas
title_full_unstemmed Effect of the excitation setup in the improved enhancement factor of covered-gold-nanorod-dimer antennas
title_sort Effect of the excitation setup in the improved enhancement factor of covered-gold-nanorod-dimer antennas
dc.creator.none.fl_str_mv Reynoso, Andrés A.
León Hilario, L. M.
Pedano, María L.
Ramos, Iván A.
author Ramos, Iván A.
author_facet Ramos, Iván A.
León Hilario, L. M.
Pedano, María L.
Reynoso, Andrés A.
author_role author
author2 León Hilario, L. M.
Pedano, María L.
Reynoso, Andrés A.
author2_role author
author
author
dc.contributor.author.fl_str_mv Ramos, Iván A.
León Hilario, L. M.
Pedano, María L.
Reynoso, Andrés A.
dc.subject.en.fl_str_mv Nanoantenna efficiency
Enhancement factor (EF)
Surface-enhancement Raman spectroscopy (SERS)
Antennas
topic Nanoantenna efficiency
Enhancement factor (EF)
Surface-enhancement Raman spectroscopy (SERS)
Antennas
https://purl.org/pe-repo/ocde/ford#2.10.00
dc.subject.ocde.es.fl_str_mv https://purl.org/pe-repo/ocde/ford#2.10.00
description Devices possessing the ability to sense both electrically and optically molecular targets are of fundamental and technological interest. Towards this end, it has been shown that covering the ends of gapped gold-nanorod-dimer nanoantennas can improve the enhancement factor (EF) that quantifies the nanoantenna efficiency for surface-enhancement Raman spectroscopy (SERS) for an incident wave coming from the top of the sample. Here, as the covering breaks the top-bottom symmetry, we investigate the behaviour of the EF for excitation coming from the bottom of the sample. This is relevant in presence of a reflecting substrate or due to the placement of the device in a cavity field. We also study the case of a superposition of waves coming from both directions in the limit cases in which a node or an antinode of the total incident field lies at the center of the gold nanorods. In all these situations we find that the EF of the covered device can continue to be higher than for the uncovered case when the geometrical parameters are tuned to the peak values of the calculated enhancement factor.
publishDate 2022
dc.date.accessioned.none.fl_str_mv 2026-03-27T21:26:17Z
dc.date.available.none.fl_str_mv 2026-03-27T21:26:17Z
dc.date.issued.fl_str_mv 2022-10
dc.type.es.fl_str_mv info:eu-repo/semantics/article
dc.type.version.es.fl_str_mv http://purl.org/coar/version/c_970fb48d4fbd8a85
format article
dc.identifier.uri.none.fl_str_mv http://hdl.handle.net/20.500.14076/29110
dc.identifier.doi.es.fl_str_mv https://doi.org/10.1039/D2CP03124H
url http://hdl.handle.net/20.500.14076/29110
https://doi.org/10.1039/D2CP03124H
dc.language.iso.en.fl_str_mv eng
language eng
dc.relation.ispartof.es.fl_str_mv CrossMark
dc.rights.es.fl_str_mv info:eu-repo/semantics/openAccess
dc.rights.uri.es.fl_str_mv http://creativecommons.org/licenses/by-nc-nd/4.0/
eu_rights_str_mv openAccess
rights_invalid_str_mv http://creativecommons.org/licenses/by-nc-nd/4.0/
dc.format.es.fl_str_mv application/pdf
dc.publisher.es.fl_str_mv Physical Chemistry Chemical Physics
dc.source.es.fl_str_mv Universidad Nacional de Ingeniería
Repositorio Institucional - UNI
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instname:Universidad Nacional de Ingeniería
instacron:UNI
instname_str Universidad Nacional de Ingeniería
instacron_str UNI
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bitstream.url.fl_str_mv http://cybertesis.uni.edu.pe/bitstream/20.500.14076/29110/2/license.txt
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spelling Ramos, Iván A.León Hilario, L. M.Pedano, María L.Reynoso, Andrés A.Reynoso, Andrés A.León Hilario, L. M.Pedano, María L.Ramos, Iván A.2026-03-27T21:26:17Z2026-03-27T21:26:17Z2022-10http://hdl.handle.net/20.500.14076/29110https://doi.org/10.1039/D2CP03124HDevices possessing the ability to sense both electrically and optically molecular targets are of fundamental and technological interest. Towards this end, it has been shown that covering the ends of gapped gold-nanorod-dimer nanoantennas can improve the enhancement factor (EF) that quantifies the nanoantenna efficiency for surface-enhancement Raman spectroscopy (SERS) for an incident wave coming from the top of the sample. Here, as the covering breaks the top-bottom symmetry, we investigate the behaviour of the EF for excitation coming from the bottom of the sample. This is relevant in presence of a reflecting substrate or due to the placement of the device in a cavity field. We also study the case of a superposition of waves coming from both directions in the limit cases in which a node or an antinode of the total incident field lies at the center of the gold nanorods. In all these situations we find that the EF of the covered device can continue to be higher than for the uncovered case when the geometrical parameters are tuned to the peak values of the calculated enhancement factor.Submitted by Quispe Rabanal Flavio (flaviofime@hotmail.com) on 2026-03-27T21:26:17Z No. of bitstreams: 1 ramos_ia.pdf: 1276417 bytes, checksum: b2fb0ae96207ebbb455b436c6edb5fc1 (MD5)Made available in DSpace on 2026-03-27T21:26:17Z (GMT). No. of bitstreams: 1 ramos_ia.pdf: 1276417 bytes, checksum: b2fb0ae96207ebbb455b436c6edb5fc1 (MD5) Previous issue date: 2022-10Este trabajo fue financiado por el Fondo Nacional de Desarrollo Científico, Tecnológico y de Innovación Tecnológica (Fondecyt - Perú) en el marco del "Diseño de Nanocontactos y Nanoantenas para Aplicaciones de Deteccion y Caracterizacion Opto-Electrónica de Moléculas" [número de contrato 174-2018]application/pdfengPhysical Chemistry Chemical PhysicsCrossMarkinfo:eu-repo/semantics/openAccesshttp://creativecommons.org/licenses/by-nc-nd/4.0/Universidad Nacional de IngenieríaRepositorio Institucional - UNIreponame:UNI-Tesisinstname:Universidad Nacional de Ingenieríainstacron:UNINanoantenna efficiencyEnhancement factor (EF)Surface-enhancement Raman spectroscopy (SERS)Antennashttps://purl.org/pe-repo/ocde/ford#2.10.00Effect of the excitation setup in the improved enhancement factor of covered-gold-nanorod-dimer antennasinfo:eu-repo/semantics/articlehttp://purl.org/coar/version/c_970fb48d4fbd8a85LICENSElicense.txtlicense.txttext/plain; charset=utf-81748http://cybertesis.uni.edu.pe/bitstream/20.500.14076/29110/2/license.txt8a4605be74aa9ea9d79846c1fba20a33MD5220.500.14076/29110oai:cybertesis.uni.edu.pe:20.500.14076/291102026-03-27 18:57:21.417Repositorio Institucional Universidad Nacional de Ingenieríarepositorio@uni.edu.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