2016
DOI: 10.1002/lpor.201500197
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Integrated all‐optical switch with 10 ps time resolution enabled by ALD

Abstract: The potential of GaAs‐based photonic crystals for fast all‐optical switching in the telecom spectral range is exploited by controlling the surface recombination and, thereby, the carrier relaxation dynamics. The structure is entirely coated with a layer of aluminium oxide using atomic layer deposition. This results in a carrier lifetime of about 10 ps, as determined by spectrally resolved pump–probe measurements. We show that the nonlinear response of the resonator is optimized when it is excited with a few‐pi… Show more

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Cited by 26 publications
(35 citation statements)
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“…Bulk recombination, due to radiative and Auger recombination, is a slow process with characteristic time scales spanning from tens to several hundreds of nanoseconds . An important carrier relaxation process in PhC structures, owing to their large surface area to volume ratio, is the surface recombination . At the surface of a semiconductor the atomic lattice is abruptly interrupted.…”
Section: Nonlinear and Dynamical Characteristics Of The Nanocavitymentioning
confidence: 99%
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“…Bulk recombination, due to radiative and Auger recombination, is a slow process with characteristic time scales spanning from tens to several hundreds of nanoseconds . An important carrier relaxation process in PhC structures, owing to their large surface area to volume ratio, is the surface recombination . At the surface of a semiconductor the atomic lattice is abruptly interrupted.…”
Section: Nonlinear and Dynamical Characteristics Of The Nanocavitymentioning
confidence: 99%
“…This results in dangling bonds, i.e., unpaired outer‐shell electrons, which introduce surface states that can trap charge carriers enhancing electron‐hole recombination . The effective carrier lifetime, τ eff , can then be written as 1τ eff =1τ rec +SLwhere τ rec is the bulk recombination rate, S is the surface recombination velocity, and L is the maximum distance to the top or bottom surface of the photonic crystal. For PhC membrane structures, L=h/2, where h is the PhC membrane thickness.…”
Section: Nonlinear and Dynamical Characteristics Of The Nanocavitymentioning
confidence: 99%
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