Geometry-induced enhancement factor improvement in covered-gold-nanorod-dimer antennas

Descripción del Articulo

Illuminated gapped-gold-nanorod dimers hold surface plasmon polaritons (SPPs) that can be engineered, by an appropriate choice of geometrical parameters, to enhance the electromagnetic field at the gap, allowing applications in molecular detection via surface-enhanced Raman spectroscopy (SERS). Envi...

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Detalles Bibliográficos
Autores: Ramos, Iván A., León Hilario, L. M., Pedano, María L., Reynoso, Andres A.
Formato: artículo
Fecha de Publicación:2021
Institución:Universidad Nacional de Ingeniería
Repositorio:UNI-Tesis
Lenguaje:inglés
OAI Identifier:oai:cybertesis.uni.edu.pe:20.500.14076/29109
Enlace del recurso:http://hdl.handle.net/20.500.14076/29109
https://doi.org/10.1039/D1RA00285F
Nivel de acceso:acceso abierto
Materia:Illuminated
Engineered
Spectroscopy of molecules
Antennas
https://purl.org/pe-repo/ocde/ford#2.10.00
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dc.title.en.fl_str_mv Geometry-induced enhancement factor improvement in covered-gold-nanorod-dimer antennas
title Geometry-induced enhancement factor improvement in covered-gold-nanorod-dimer antennas
spellingShingle Geometry-induced enhancement factor improvement in covered-gold-nanorod-dimer antennas
Ramos, Iván A.
Illuminated
Engineered
Spectroscopy of molecules
Antennas
https://purl.org/pe-repo/ocde/ford#2.10.00
title_short Geometry-induced enhancement factor improvement in covered-gold-nanorod-dimer antennas
title_full Geometry-induced enhancement factor improvement in covered-gold-nanorod-dimer antennas
title_fullStr Geometry-induced enhancement factor improvement in covered-gold-nanorod-dimer antennas
title_full_unstemmed Geometry-induced enhancement factor improvement in covered-gold-nanorod-dimer antennas
title_sort Geometry-induced enhancement factor improvement in covered-gold-nanorod-dimer antennas
dc.creator.none.fl_str_mv Reynoso, Andres 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, Andres A.
author_role author
author2 León Hilario, L. M.
Pedano, María L.
Reynoso, Andres A.
author2_role author
author
author
dc.contributor.author.fl_str_mv Ramos, Iván A.
León Hilario, L. M.
Pedano, María L.
Reynoso, Andres A.
dc.subject.en.fl_str_mv Illuminated
Engineered
Spectroscopy of molecules
Antennas
topic Illuminated
Engineered
Spectroscopy of molecules
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 Illuminated gapped-gold-nanorod dimers hold surface plasmon polaritons (SPPs) that can be engineered, by an appropriate choice of geometrical parameters, to enhance the electromagnetic field at the gap, allowing applications in molecular detection via surface-enhanced Raman spectroscopy (SERS). Envisioning hybrid devices in which the SERS spectroscopy of molecules in the gap is complemented by electrical measurements, it arises the question of designing efficient geometries to contact the nanorods without decreasing the enhancement factor (EF) of the nanoantenna, i.e., the figure of merit for SERS spectroscopy. Within this framework we theoretically study the feasibility to fabricate designs based on covering with gold the far-from-the-gap areas of the dimer. We show that by tuning the geometrical parameters of the designs these systems can reach enhancement factors larger than the best achieved in the uncovered dimer: this supremacy survives even in the presence of dimer asymmetries and vacancies at the interfaces between the nanorods and the covering layers. Our results show that geometrical modifications away from the gap can improve the optical response at the gap, thus enabling the use of these devices both for hybrid and optical applications.
publishDate 2021
dc.date.accessioned.none.fl_str_mv 2026-03-27T20:31:02Z
dc.date.available.none.fl_str_mv 2026-03-27T20:31:02Z
dc.date.issued.fl_str_mv 2021-03
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
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dc.identifier.uri.none.fl_str_mv http://hdl.handle.net/20.500.14076/29109
dc.identifier.doi.es.fl_str_mv https://doi.org/10.1039/D1RA00285F
url http://hdl.handle.net/20.500.14076/29109
https://doi.org/10.1039/D1RA00285F
dc.language.iso.en.fl_str_mv eng
language eng
dc.relation.ispartof.es.fl_str_mv CrossMark
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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 RSC Advances
dc.source.es.fl_str_mv Universidad Nacional de Ingeniería
Repositorio Institucional - UNI
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spelling Ramos, Iván A.León Hilario, L. M.Pedano, María L.Reynoso, Andres A.Reynoso, Andres A.León Hilario, L. M.Pedano, María L.Ramos, Iván A.2026-03-27T20:31:02Z2026-03-27T20:31:02Z2021-03http://hdl.handle.net/20.500.14076/29109https://doi.org/10.1039/D1RA00285FIlluminated gapped-gold-nanorod dimers hold surface plasmon polaritons (SPPs) that can be engineered, by an appropriate choice of geometrical parameters, to enhance the electromagnetic field at the gap, allowing applications in molecular detection via surface-enhanced Raman spectroscopy (SERS). Envisioning hybrid devices in which the SERS spectroscopy of molecules in the gap is complemented by electrical measurements, it arises the question of designing efficient geometries to contact the nanorods without decreasing the enhancement factor (EF) of the nanoantenna, i.e., the figure of merit for SERS spectroscopy. Within this framework we theoretically study the feasibility to fabricate designs based on covering with gold the far-from-the-gap areas of the dimer. We show that by tuning the geometrical parameters of the designs these systems can reach enhancement factors larger than the best achieved in the uncovered dimer: this supremacy survives even in the presence of dimer asymmetries and vacancies at the interfaces between the nanorods and the covering layers. Our results show that geometrical modifications away from the gap can improve the optical response at the gap, thus enabling the use of these devices both for hybrid and optical applications.Submitted by Quispe Rabanal Flavio (flaviofime@hotmail.com) on 2026-03-27T20:31:02Z No. of bitstreams: 1 ramos_ia.pdf: 1276417 bytes, checksum: b2fb0ae96207ebbb455b436c6edb5fc1 (MD5)Made available in DSpace on 2026-03-27T20:31:02Z (GMT). No. of bitstreams: 1 ramos_ia.pdf: 1276417 bytes, checksum: b2fb0ae96207ebbb455b436c6edb5fc1 (MD5) Previous issue date: 2021-03Este 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 174-2018application/pdfengRSC AdvancesCrossMarkinfo:eu-repo/semantics/openAccesshttp://creativecommons.org/licenses/by-nc-nd/4.0/Universidad Nacional de IngenieríaRepositorio Institucional - UNIreponame:UNI-Tesisinstname:Universidad Nacional de Ingenieríainstacron:UNIIlluminatedEngineeredSpectroscopy of moleculesAntennashttps://purl.org/pe-repo/ocde/ford#2.10.00Geometry-induced enhancement factor improvement in covered-gold-nanorod-dimer antennasinfo:eu-repo/semantics/articlehttp://purl.org/coar/version/c_970fb48d4fbd8a85TEXTramos_ia.pdf.txtramos_ia.pdf.txtExtracted texttext/plain48026http://cybertesis.uni.edu.pe/bitstream/20.500.14076/29109/3/ramos_ia.pdf.txt2d8bc513875e2c922c25e87182939eeeMD53LICENSElicense.txtlicense.txttext/plain; charset=utf-81748http://cybertesis.uni.edu.pe/bitstream/20.500.14076/29109/2/license.txt8a4605be74aa9ea9d79846c1fba20a33MD52ORIGINALramos_ia.pdframos_ia.pdfapplication/pdf1276417http://cybertesis.uni.edu.pe/bitstream/20.500.14076/29109/1/ramos_ia.pdfb2fb0ae96207ebbb455b436c6edb5fc1MD5120.500.14076/29109oai:cybertesis.uni.edu.pe:20.500.14076/291092026-03-28 03:10:21.275Repositorio Institucional Universidad Nacional de Ingenieríarepositorio@uni.edu.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