2018
DOI: 10.1364/oe.26.014982
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Mapping the electric field distribution of tightly focused cylindrical vector beams with gold nanorings

Abstract: In this paper gold nanorings (NRs) are applied as particularly well-suited sensing elements for mapping the radially symmetric electric fields in the high numerical aperture focus of cylindrical vector beams. The optical properties of gold nanorings are analyzed by a combination of extinction and single particle dark field spectroscopy as well as confocal photoluminescence (PL) imaging. The results are compared to numerical calculations. The in-plane components in the focus of the cylindrical vector beams are … Show more

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Cited by 8 publications
(7 citation statements)
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“…The pattern shape strongly depends on the excitation wavelength and excitation doughnut mode. Even though both the TPR mode and interband transitions can be excited by 530 nm photons, we can exclude that TPR excitation significantly contributes to the PL emission, since the pattern shapes indicate an isotropic excitation and reflect the electric field distribution of the focused beam . One might argue that LPR could also be excited directly by the 530 nm laser and thus cause an isotropic excitation pattern.…”
Section: Resultsmentioning
confidence: 98%
“…The pattern shape strongly depends on the excitation wavelength and excitation doughnut mode. Even though both the TPR mode and interband transitions can be excited by 530 nm photons, we can exclude that TPR excitation significantly contributes to the PL emission, since the pattern shapes indicate an isotropic excitation and reflect the electric field distribution of the focused beam . One might argue that LPR could also be excited directly by the 530 nm laser and thus cause an isotropic excitation pattern.…”
Section: Resultsmentioning
confidence: 98%
“…VLS nanowire growth is carried out in a quartz tube furnace with precursor gas mixture of H2 (270 sccm) and of SiH4 (30 sccm), at a pressure of 100 mbar. Silicon shell growth is done at a temperature of 520 °C with a gas mixture of H2 ( Using a home built parabolic mirror (NA: 0.998) [32] assisted setup, we achieve a diffraction-limited confocal resolution by illumination with a radially polarized laser beam [33]. With a 636.3 nm diode laser operating in continuous wave mode we obtain a focus diameter of roughly ~300 nm [34].…”
Section: Methodsmentioning
confidence: 99%
“…Using a custom-built setup with a parabolic mirror (NA: 0.998) [ 34 ], we achieve a diffraction-limited confocal resolution by illumination with a radially polarized laser beam [ 35 ]. With a 636.3 nm diode laser operating in continuous-wave mode we obtain a focus diameter of roughly 300 nm [ 36 ].…”
Section: Methodsmentioning
confidence: 99%