2015
DOI: 10.1021/acs.nanolett.5b00574
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Efficient Coupling of an Antenna-Enhanced nanoLED into an Integrated InP Waveguide

Abstract: Increasing power consumption in traditional on-chip metal interconnects has made optical links an attractive alternative. However, such a link is currently missing a fast, efficient, nanoscale light-source. Coupling nanoscale optical emitters to optical antennas has been shown to greatly increase their spontaneous emission rate and efficiency. Such a structure would be an ideal emitter for an on-chip optical link. However, there has never been a demonstration of an antenna-enhanced emitter coupled to a low-los… Show more

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Cited by 27 publications
(12 citation statements)
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References 36 publications
(42 reference statements)
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“…Note, in addition, the presence of a sharp change at h = 110 nm for all d values. We attribute this to optical coupling to the polymer layer produced by the resulting 10 nm nanogap between the top metal layer and the metal disk [ 30 , 31 ]. Light leaked to the polymer layer may affect the field intensity associated with the metal/air SPR (peak A) and, therefore, to the surface sensitivity and the resonance dip amplitude.…”
Section: Resultsmentioning
confidence: 99%
“…Note, in addition, the presence of a sharp change at h = 110 nm for all d values. We attribute this to optical coupling to the polymer layer produced by the resulting 10 nm nanogap between the top metal layer and the metal disk [ 30 , 31 ]. Light leaked to the polymer layer may affect the field intensity associated with the metal/air SPR (peak A) and, therefore, to the surface sensitivity and the resonance dip amplitude.…”
Section: Resultsmentioning
confidence: 99%
“…Differently from nanolasers, nanoLEDs do not require a lasing threshold and therefore do not need a high-Q cavity, resulting in much lower current operation requirements [32]. Importantly, in recent years several advances have been made to increase the efficiency of nanoLEDs towards >10% which include Purcell enhancement of radiative emission [33][34][35], suppression of nonradiative surface effects via chemical passivation treatments [36], and efficient waveguidecoupling methods [37,38]. NanoLEDs have been already demonstrated for a photonic crystal (PhC) LED [39], a plasmonic LED [40] and a waveguide-coupled nanoLED [37], showing output power levels in the order of tens to hundreds of pW for the PhC case and up to 300 nW for the waveguide-coupled case.…”
Section: Introductionmentioning
confidence: 99%
“…The activation of the all-or-nothing optical spiking response (called excitable) is achieved via high-speed nonlinear electrical modulation of the nanoLED. Importantly, the sub-λ metal-cavity offers strong light-matter interaction at the nanoscale via the Purcell effect [30], which scales inversely with the mode volume [31,38], leading to faster and more efficient light emission and of advantage for high-bandwidth optical spiking. Using a model that combines the dynamical equations of the circuit and rate equations, and using realistic parameters of a nanodevice that takes into account material parameters, nonradiative effects and size scaling, we analyze the characteristics of the fired optical spikes.…”
Section: Introductionmentioning
confidence: 99%
“…Optical antennas exploit the unique properties of metal nanostructures that exhibit strong coupling of electronic plasma to electromagnetic radiation at optical frequencies. These antennas can direct electromagnetic waves in sub-wavelength-scale devices, for applications such as near-field optical microscopy [20]- [23], surface-enhanced Raman spectroscopy [13]- [17], [24], surface enhanced infrared absorption spectroscopy [25], [26], and photovoltaics [27], and devices such as nanoLEDs [28], [29].…”
Section: Introductionmentioning
confidence: 99%