2016
DOI: 10.1364/oe.24.015965
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Monolithic AlGaAs second-harmonic nanoantennas

Abstract: We demonstrate monolithic aluminum gallium arsenide (AlGaAs) optical anoantennas.Using a selective oxidation technique, we fabricate such epitaxial semiconductor nanoparticles on an aluminum oxide substrate. Second harmonic generation from an AlGaAs nanocylinder of height h=400 nm and varying radius pumped with femtosecond pulses delivered at 1554-nm wavelength has been measured, revealing a peak conversion efficiency exceeding 10 -5 for nanocylinders with an otpimized geometry.

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Cited by 233 publications
(258 citation statements)
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(31 reference statements)
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“…This corresponds to 1.5 × 10 5 enhancement of the THG signal relative to that from an unstructured Si film with the same thickness. Recent demonstrations also include enhancement of SHG in resonant nanopillars made of the high-index noncentrosymmetric III-V semiconductors GaAs (60) and AlGaAs (61). An enhancement factor of 10 4 relative to unstructured GaAs films is shown with total conversion efficiency of 2 × 10 −5 at a pump intensity of 3.4 GW/cm 2 .…”
Section: Nonlinear Optics With Resonant Dielectric Nanostructuresmentioning
confidence: 99%
“…This corresponds to 1.5 × 10 5 enhancement of the THG signal relative to that from an unstructured Si film with the same thickness. Recent demonstrations also include enhancement of SHG in resonant nanopillars made of the high-index noncentrosymmetric III-V semiconductors GaAs (60) and AlGaAs (61). An enhancement factor of 10 4 relative to unstructured GaAs films is shown with total conversion efficiency of 2 × 10 −5 at a pump intensity of 3.4 GW/cm 2 .…”
Section: Nonlinear Optics With Resonant Dielectric Nanostructuresmentioning
confidence: 99%
“…We find that the SHG yield at the anapole mode in these hybrid platforms is almost two orders of magnitude higher than in isolated nanopillars. We also find sizeable THG with an emission yield comparable to that of SHG, which is unexpected since third-order nonlinear processes are commonly negligible in these systems [28,38]. The polarization-dependent optical properties of this platform together with the SHG angular emission characteristics indicate an improvement in both pump coupling and emission efficiency.…”
Section: Introductionmentioning
confidence: 59%
“…In this experiment we fully characterized the nonlinear emission from individual nanostructures, by using the nonlinear confocal setup described in the Experimental section (see also [28,33,38]). In brief, each individual nanoantenna is addressed with ultrashort pump pulses (140 fs) centered at 1554 nm and focused down to the diffraction limit by a 0.85 NA objective.…”
Section: Resultsmentioning
confidence: 99%
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