2021
DOI: 10.1021/acs.jpcc.1c08402
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Revealing the Three-Dimensional Orientation and Interplay between Plasmons and Interband Transitions for Single Gold Bipyramids by Photoluminescence Excitation Pattern Imaging

Abstract: Gold bipyramids (AuBPs) attract significant attention due to the large enhancement of the electric field around their sharp tips and well-defined tunability of their plasmon resonances. Excitation patterns of single AuBPs are recorded using raster-scanning confocal microscopy combined with radially and azimuthally polarized laser beams. Photoluminescence spectra (PL) and excitation patterns of the same AuBPs are acquired with three different excitation wavelengths. The isotropic excitation patterns suggest tha… Show more

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Cited by 3 publications
(2 citation statements)
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“…In particular, if the excitation frequency ω 0 is close to resonance with a longitudinal antenna mode, then K z (ω 0 ) ≫ K xy (ω 0 ) and the Raman signal will be strongest when the sample position r matches a maximum of I bg z ( r , ϵ); conversely, if ω 0 is close to resonance with a transverse antenna mode, then K z (ω 0 ) ≪ K xy (ω 0 ) and the Raman signal will be strongest when the sample position r matches a maximum of I bg xy ( r , ϵ). This discussion allows us to interpret the experimental confocal Raman maps by connecting them to the near-field distribution of the focused excitation beam and the transverse vs longitudinal nature of the antenna mode that is associated with each plasmonic gap mode.…”
Section: Resultsmentioning
confidence: 99%
“…In particular, if the excitation frequency ω 0 is close to resonance with a longitudinal antenna mode, then K z (ω 0 ) ≫ K xy (ω 0 ) and the Raman signal will be strongest when the sample position r matches a maximum of I bg z ( r , ϵ); conversely, if ω 0 is close to resonance with a transverse antenna mode, then K z (ω 0 ) ≪ K xy (ω 0 ) and the Raman signal will be strongest when the sample position r matches a maximum of I bg xy ( r , ϵ). This discussion allows us to interpret the experimental confocal Raman maps by connecting them to the near-field distribution of the focused excitation beam and the transverse vs longitudinal nature of the antenna mode that is associated with each plasmonic gap mode.…”
Section: Resultsmentioning
confidence: 99%
“…Special interest has been given to geometries featuring spikes, tips, and edges such as, e.g., bi-pyramids, cones, or star-shaped nanoparticles (s-NPs): in the sharpest regions, light excitation produces electromagnetic hot spots where radiation is highly confined and extreme field enhancements can be attained. Because of these intense near fields induced at their hot spots, spiky nanostructures show enhanced sensitivity to their local environment and, as such, have gained great attention, e.g., in surface-enhanced Raman spectroscopy, biochemical sensing and applications, and surface chemistry. …”
Section: Introductionmentioning
confidence: 99%