Generating Ultrabroadband Deep-UV Radiation and Sub-10 nm Gap by Hybrid-Morphology Gold Antennas
- Liping Shi*Liping Shi*E-mail: [email protected]Institute of Quantum Optics, Leibniz University Hannover, Welfengarten 1, 30167, Hannover, GermanyCluster of Excellence PhoenixD (Photonics, Optics, and Engineering-Innovation Across Disciplines), 30167, Hannover, GermanyMore by Liping Shi
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- José R. C. Andrade*José R. C. Andrade*E-mail: [email protected]Institute of Quantum Optics, Leibniz University Hannover, Welfengarten 1, 30167, Hannover, GermanyCluster of Excellence PhoenixD (Photonics, Optics, and Engineering-Innovation Across Disciplines), 30167, Hannover, GermanyMore by José R. C. Andrade
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- Ayhan TajalliAyhan TajalliInstitute of Quantum Optics, Leibniz University Hannover, Welfengarten 1, 30167, Hannover, GermanyCluster of Excellence PhoenixD (Photonics, Optics, and Engineering-Innovation Across Disciplines), 30167, Hannover, GermanyMore by Ayhan Tajalli
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- Jiao Geng*Jiao Geng*E-mail: [email protected]Institute of Quantum Optics, Leibniz University Hannover, Welfengarten 1, 30167, Hannover, GermanyMore by Jiao Geng
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- Juemin YiJuemin YiInstitute of Physics and Center of Interface Science, Carl von Ossietzky University Oldenburg, 26129, Oldenburg, GermanyMore by Juemin Yi
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- Torsten HeidenblutTorsten HeidenblutCluster of Excellence PhoenixD (Photonics, Optics, and Engineering-Innovation Across Disciplines), 30167, Hannover, GermanyInstitute of Materials Science, Leibniz University Hannover, An der University 2, 30823, Garbsen, Hannover GermanyMore by Torsten Heidenblut
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- Frans B. SegerinkFrans B. SegerinkOptical Sciences, MESA+ Institute for Nanotechnology, University of Twente, P.O. Box 217, 7500AE Enschede, The NetherlandsMore by Frans B. Segerink
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- Ihar BabushkinIhar BabushkinInstitute of Quantum Optics, Leibniz University Hannover, Welfengarten 1, 30167, Hannover, GermanyCluster of Excellence PhoenixD (Photonics, Optics, and Engineering-Innovation Across Disciplines), 30167, Hannover, GermanyMore by Ihar Babushkin
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- Maria KholodtsovaMaria KholodtsovaLIDYL, CEA, CNRS, Universite Paris-Saclay, CEA Saclay 91191, Gif-sur-Yvette, FranceMore by Maria Kholodtsova
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- Hamed MerdjiHamed MerdjiLIDYL, CEA, CNRS, Universite Paris-Saclay, CEA Saclay 91191, Gif-sur-Yvette, FranceMore by Hamed Merdji
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- Bert BastiaensBert BastiaensLaser Physics and Nonlinear Optics, MESA+ Institute for Nanotechnology, University of Twente, 7500AE Enschede, The NetherlandsMore by Bert Bastiaens
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- Uwe MorgnerUwe MorgnerInstitute of Quantum Optics, Leibniz University Hannover, Welfengarten 1, 30167, Hannover, GermanyCluster of Excellence PhoenixD (Photonics, Optics, and Engineering-Innovation Across Disciplines), 30167, Hannover, GermanyMore by Uwe Morgner
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- Milutin Kovacev*Milutin Kovacev*E-mail: [email protected]Institute of Quantum Optics, Leibniz University Hannover, Welfengarten 1, 30167, Hannover, GermanyCluster of Excellence PhoenixD (Photonics, Optics, and Engineering-Innovation Across Disciplines), 30167, Hannover, GermanyMore by Milutin Kovacev
Abstract

We experimentally investigate the interaction between hybrid-morphology gold optical antennas and a few-cycle Ti:sapphire laser up to ablative intensities, demonstrating rich nonlinear plasmonic effects and promising applications in coherent frequency upconversion and nanofabrication technology. The two-dimensional array of hybrid antennas consists of elliptical apertures combined with bowties in its minor axis. The plasmonic resonance frequency of the bowties is red-shifted with respect to the laser central frequency and thus mainly enhances the third harmonic spectrum at long wavelengths. The gold film between two neighboring elliptical apertures forms an hourglass-shaped structure, which acts as a “plasmonic lens” and thus strongly reinforces surface currents into a small area. This enhanced surface current produces a rotating magnetic field that deeply penetrates into the substrate. At resonant frequency, the magnetic field is further intensified by the bowties. The resonant frequency of the hourglass is blueshifted with respect to the laser central frequency. Consequently, it spectacularly extends the third harmonic spectrum toward short wavelengths. The resultant third harmonic signal ranges from 230 to 300 nm, much broader than the emission from a sapphire crystal. In addition, the concentration of surface current within the neck of the hourglass antenna results in a structural modification through laser ablation, producing sub-10 nm sharp metallic gaps. Moreover, after laser illumination the optical field hotspots are imprinted around the antennas, allowing us to confirm the subwavelength enhancement of the electric near-field intensity.
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