2012
DOI: 10.1088/1367-2630/14/2/023035
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Fano-like interference of plasmon resonances at a single rod-shaped nanoantenna

Abstract: Single metallic nanorods acting as half-wave antennas in the optical range exhibit an asymmetric, multi-resonant scattering spectrum that strongly depends on both their length and dielectric properties. Here we show that such spectral features can be easily understood in terms of Fano-like interference between adjacent plasmon resonances. On the basis of analytical and numerical results for different geometries, we demonstrate that Fano resonances may appear for such single-particle nanoantennas provided that … Show more

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Cited by 59 publications
(80 citation statements)
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“…When two oscillators overlap both spatially and spectrally, both constructive and destructive interferences can be observed [16]. Destructive interference can result in reduced scattering cross sections and generate strongly localized near-fields [17], while constructive interference can result in super-radiant modes with enhanced scattering [12].…”
Section: Introductionmentioning
confidence: 99%
“…When two oscillators overlap both spatially and spectrally, both constructive and destructive interferences can be observed [16]. Destructive interference can result in reduced scattering cross sections and generate strongly localized near-fields [17], while constructive interference can result in super-radiant modes with enhanced scattering [12].…”
Section: Introductionmentioning
confidence: 99%
“…This phenomenon, characterized by an asymmetric spectral line shape, is known as Fano resonance or Fano interference and mainly arises here from the Q y mode's l = 3 component, as it is also observed for nanorods (α = 180°). 39 The impact of this Fano interference on the angular distribution of the scattering intensity is illustrated in Figure 2. In this figure, simulated (panels a,b) and experimental (panel c) results for the L = 250 nm, α = 120°antenna in Figure 1 are provided, at several wavelengths around the Q y -Fano resonance for y-polarized light.…”
mentioning
confidence: 99%
“…5.a). Thus, phase toggling takes place as the photon energy is varied through the coupled quadrupole resonance, 55 Placing the two particles at larger distance (black line in Fig 5.b) the coupling is reduced and the extinction spectrum shows a broad peak, resembling to the dipolar excitation of a single particle. If a third particle is located at the center of such dimer, the dipolar mode is only slightly perturbated since the field acting on the central particle at the origin vanishes and the resonance is still broad.…”
Section: Resultsmentioning
confidence: 99%