2018
DOI: 10.1515/zpch-2018-1109
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Single Particle Spectroscopy of Radiative Processes in Colloid-to-Film-Coupled Nanoantennas

Abstract: We present a fluorescent emitter (rhodamine B) coupled to a dielectric or metallic interface as well as a metallic cavity to study their radiative decay processes. Supported by finite-difference time-domain (FDTD) simulations, we correlate the non-radiative and radiative decay rates with the absorption and scattering cross section efficiencies, respectively. On a single particle level, we use atomic force microscopy (AFM), scanning electron microscopy (SEM), scattering spectroscopy, fluorescence life time imag… Show more

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Cited by 7 publications
(5 citation statements)
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“…Our findings pave the way for further exploitation of plasmonic nanoparticle chains as waveguides and photonic devices. For example, the waveguide mode can be intervened at each contact point by inserting materials such as fluorescent emitters 46 and organic 47 or smart polymers 48 to further modulate and enhance the radiative properties of the plasmonic waveguide. 49 Of particular interest is the coupling at end points of the chain, which sustain particular edge states that may be tuned by complex chain geometries (e.g., bipartite chains).…”
Section: Nano Lettersmentioning
confidence: 99%
“…Our findings pave the way for further exploitation of plasmonic nanoparticle chains as waveguides and photonic devices. For example, the waveguide mode can be intervened at each contact point by inserting materials such as fluorescent emitters 46 and organic 47 or smart polymers 48 to further modulate and enhance the radiative properties of the plasmonic waveguide. 49 Of particular interest is the coupling at end points of the chain, which sustain particular edge states that may be tuned by complex chain geometries (e.g., bipartite chains).…”
Section: Nano Lettersmentioning
confidence: 99%
“…One of the most promising ways to employ plasmonic cavities is their impact on the emitters’ decay channels. Due to the QDs’ close proximity to the metal surfaces, the excitable states of the quantum dots are altered, leading to both faster radiative and nonradiative decays . Since the increase in radiative decay rates generally exceeds that of the nonradiative channels, the overall quantum efficiency of the QD emission improves significantly.…”
Section: Resultsmentioning
confidence: 99%
“…The quantum yield (QD) of the assembled structures was estimated up to 25% (see Section T2 in the Supporting Information). [ 38 ]…”
Section: Methodsmentioning
confidence: 99%
“…The quantum yield (QD) of the assembled structures was estimated up to 25% (see Section T2 in the Supporting Information). [38] Confocal Fluorescence Microscopy: Confocal fluorescence microscopy (CFM) measurements were acquired with an inverted confocal scanning microscope (MicroTime 200, PicoQuant, Germany) with a 100× air objective (UPLFLN, NA 0.9, Olympus, Japan). For excitation, a picosecond pulsed p-polarized laser diode source (LDH-D-C-405, PicoQuant, Germany) with a center wavelength of 405 nm and a pulse width of 110 ps (full width at half-maximum, FWHM), driven at a repetition rate of 0.5 MHz.…”
Section: Fabrication Of Gold Gratingsmentioning
confidence: 99%