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dc.contributor.authorCsete, , M.
dc.contributor.authorSzenes, A.
dc.contributor.authorToth, E.
dc.contributor.authorVass, D.
dc.contributor.authorFekete, O.
dc.contributor.authorBanhelyi, B.
dc.contributor.authorPapp, Istvan
dc.contributor.authorBiró, Tamás S.
dc.contributor.authorCsernai, László Pál
dc.contributor.authorKroo, N
dc.date.accessioned2022-06-21T13:00:23Z
dc.date.available2022-06-21T13:00:23Z
dc.date.created2022-05-02T09:36:51Z
dc.date.issued2022
dc.identifier.issn1557-1955
dc.identifier.urihttps://hdl.handle.net/11250/2999862
dc.description.abstractPlasmonic nanoresonators of core–shell composition and nanorod shape were optimized to tune their absorption cross-section maximum to the central wavelength of a short laser pulse. The number density distribution of randomly located nanoresonators along a laser pulse-length scaled target was numerically optimized to maximize the absorptance with the criterion of minimal absorption difference between neighboring layers illuminated by two counter-propagating laser pulses. Wide Gaussian number density distribution of core–shell nanoparticles and nanorods enabled to improve the absorptance with low standard deviation; however, the energy deposited until the overlap of the two laser pulses exhibited a considerable standard deviation. Successive adjustment resulted in narrower Gaussian number density distributions that made it possible to ensure almost uniform distribution of the deposited energy integrated until the maximal overlap of the two laser pulses. While for core–shell nanoparticles the standard deviation of absorptance could be preserved, for the nanorods it was compromised. Considering the larger and polarization independent absorption cross-section as well as the simultaneously achievable smaller standard deviation of absorptance and deposited energy distribution, the core–shell nanoparticles outperform the nanorods both in optimized and adjusted nanoresonator distributions. Exception is the standard deviation of deposited energy distribution considered for the complete layers that is smaller in the adjusted nanorod distribution. Optimization of both nanoresonator distributions has potential applications, where efficient and uniform energy deposition is crucial, including biomedical applications, phase transitions, and even fusion.en_US
dc.language.isoengen_US
dc.publisherSpringeren_US
dc.rightsNavngivelse 4.0 Internasjonal*
dc.rights.urihttp://creativecommons.org/licenses/by/4.0/deed.no*
dc.titleComparative study on the uniform energy deposition achievable via optimized plasmonic nanoresonator distributionsen_US
dc.typeJournal articleen_US
dc.typePeer revieweden_US
dc.description.versionpublishedVersionen_US
dc.rights.holderCopyright 2022 The Author(s)en_US
cristin.ispublishedtrue
cristin.fulltextoriginal
cristin.qualitycode1
dc.identifier.doi10.1007/s11468-021-01571-x
dc.identifier.cristin2020506
dc.source.journalPlasmonicsen_US
dc.source.pagenumber775-787en_US
dc.relation.projectNorges forskningsråd: 255253en_US
dc.identifier.citationPlasmonics. 2022, 17, 775-787.en_US
dc.source.volume17en_US


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