Abstract

We study the angular emission of a single emitter near a metallic nanoparticle by experiments and numerical calculations. In the experiments, a single fluorescent molecule is controllably scanned near an optical monopole antenna. Large changes in the angular emission of the molecule occur due to the coupling to the particle. Both the polarization and intensity of the angular emission show a distinct dependence on the particle plasmon resonance and on the relative positions and orientations of the emitter and particle. These changes strongly modify the collection efficiency, particularly for objectives of limited numerical aperture; it is important to take the collection system into account fully in the interpretation of enhanced fluorescence and when comparing measurements on ensembles to reference situations. Unlike for ensembles, by addressing a single emitter of well-defined orientation the angular emission is naturally separated from absolute intensities. By dynamically controlling the emitter position a clean reference is then established. This allows all results to be interpreted directly as the coupling of an emitter dipole moment to the dipolar plasmon mode of the antenna. The emitter couples to the antenna mode, which in turn couples to the radiation field, thus determining the angular emission.

Highlights

  • Optical antennas and angular emissionWe have experimentally shown that the angular emission of a single molecule, i.e. the far-field electric field amplitude, phase and polarization as a function of angle, can be controlled by coupling to resonant modes of optical antennas [7, 15]

  • We study the angular emission of a single emitter near a metallic nanoparticle by experiments and numerical calculations

  • The angular emission of an emitter can be drastically altered by coupling to the plasmon resonance of a metallic nanoparticle

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Summary

Optical antennas and angular emission

We have experimentally shown that the angular emission of a single molecule, i.e. the far-field electric field amplitude, phase and polarization as a function of angle, can be controlled by coupling to resonant modes of optical antennas [7, 15]. For a single emitter of well-defined orientation and controlled position, the angular emission is naturally decoupled from absolute intensities and a clear reference is obtained This allows all results presented to be interpreted directly and to be explained in a straightforward way as the coupling of the emitter dipole to dipolar antenna plasmon modes; direct insight into the role of the antenna plasmon resonance in the emission process is gained

Calculation of decay rates and angular directivity
The role of the plasmon resonance in the angular emission
Calculations for two antennas
The collection efficiency
Vertical antenna
Horizontal antenna
Conclusions
Full Text
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