2017
DOI: 10.1364/josab.34.000691
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Lattice modes and plasmonic linewidth engineering in gold and aluminum nanoparticle arrays

Abstract: International audienc

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Cited by 174 publications
(160 citation statements)
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“…Figure b shows the first and second‐order Bragg diffraction from a 2D nanohole array written in PDMS with a varying lattice constant ( a = 420, 440, 500 nm). In contrast to the plasmonic mode (Figure a), the line width of these photonic modes is comparably narrow …”
Section: Spectroscopic Properties Of Tunable Plasmonic Latticesmentioning
confidence: 89%
See 1 more Smart Citation
“…Figure b shows the first and second‐order Bragg diffraction from a 2D nanohole array written in PDMS with a varying lattice constant ( a = 420, 440, 500 nm). In contrast to the plasmonic mode (Figure a), the line width of these photonic modes is comparably narrow …”
Section: Spectroscopic Properties Of Tunable Plasmonic Latticesmentioning
confidence: 89%
“…The ordered arrays possess the combined properties of particle plasmons and diffractive modes (see Figure c), also known as plasmonic hybridization . At the SLR conditions the incoming light is trapped inside the lattice plane and leads to a narrow full width at half maximum (FWHM or line width) and strongly enhanced local electric fields at the nanoparticle surface . This occurs due to the constructive interference and coherent coupling at the SLR position which leads to the standing wave formation and hence allows for localized field enhancement.…”
Section: Spectroscopic Properties Of Tunable Plasmonic Latticesmentioning
confidence: 99%
“…As the SERS enhancement [133] equals ðjEj=jE 0 jÞ 4 , this means that a two-dimensional nanoantenna lattice with a 40-nm spacing would enhance the SERS signal over 44% of the surface area of the specimen [π · ð15 nmÞ 2 =ð40 nmÞ 2 ¼ 0.44], with a factor of between 10 3 and 10 6 . In addition (if the spacing is above but on the same order of magnitude as the wavelength of the incident light), diffractive coupling between the ion-beam-shaped nanoparticles can (under the right incident conditions) lead to the creation of lattice-surface modes [134], which, in their spectral response of the IBSNA, manifest themselves as Fano resonances [134][135][136] and which can be tuned by the nanoantenna shape, orientation, and spacing [134,[137][138][139]. In contrast to the resonances of the individual nanoantennas, which usually feature quality factors smaller LOCALIZED PLASMONIC RESONANCES OF PROLATE … PHYS.…”
Section: B Ibsnas For Surface-enhanced Raman Spectroscopy (Sers)mentioning
confidence: 99%
“…REV. APPLIED 9, 064038 (2018) 064038-15 than 10, the quality factors of Fano resonances can reach several hundred [134,138,139], which can be exploited for very selective molecule detection in SERS applications.…”
Section: B Ibsnas For Surface-enhanced Raman Spectroscopy (Sers)mentioning
confidence: 99%
“…One of the loss mitigating strategies in noble-metal plasmonics involves near-or far-field coupling of nanostructures. In periodic two-dimensional nanoparticle arrays, for instance, radiative coupling between diffracted waves in the array plane and localized surface plasmon resonances (LSPRs) produces collective surface lattice resonances (SLRs) [16][17][18][19]. The full-width at half maximum (FWHM) of SLRs in Au or Ag nanoparticle arrays can be <10 nm [19], which is a significant improvement from 80 -100 nm for LSPRs in isolated nanostructures of these noble metals.…”
Section: Introductionmentioning
confidence: 99%