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arXiv:2004.13168 · Optics Letters

High spectro-temporal purity single-photons from silicon micro-racetrack resonators using a dual-pulse configuration

Ben M. Burridge, Imad I. Faruque, John G. Rarity, Jorge Barreto

Published May 12, 2020• 29 citations
arXivHTMLPDF

Abstract

Single-photons with high spectro-temporal purity are an essential resource for quantum photonic technologies. The highest reported purity up until now from a conventional silicon photonic device is 92% without any spectral filtering. We have experimentally generated and observed single-photons with 98.0 ± 0.3 % spectro-temporal purity, an upper bound of the stimulated emission tomography, using a conventional micro-racetrack resonator and an engineered dual pump pulse.

DOI
10.1364/ol.393077

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Single-photons with high spectro-temporal purity are an essential resource for quantum photonic technologies. The highest reported purity up until now from a conventional silicon photonic device is 92% without any spectral filtering. We have experimentally generated and observed single-photons with 98.0 ± 0.3 % spectro-temporal purity, an upper bound of the stimulated emission tomography, using a conventional micro-racetrack resonator and an engineered dual pump pulse.
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Recently, many researchers focus on the integration of single photon sources on an optical chip toward the realization of large-scale quantum information processing.Identical single photons are required to obtain good interference between photons for quantum information processing, for which high "spectral purity" of single photons is required.An appealing scheme is employing the spontaneous four-wave mixing (SFWM) in a silicon micro-ring resonator (MRR) because it allows us to generate high-purity photons without external spectral filters.However, the purity value is limited to 0.92 due to the dispersion property of an MRR We have developed a new scheme to further increase the spectral purity from an MRR by manipulating the spectral phase distribution of the pump pulse.Via exploring several strategies on the spectral phase modulation, we found that the purity of single photon can be increased up to approximately 0.96 breaking the conventional limitation of 0.92 in a standard MRR.We further explore the experimental feasibility of the scheme toward future implementation.
We experimentally demonstrate a high-spectral-purity photon source by designing a dual-Mach–Zehnder-interferometer-coupled silicon ring resonator, wherein the linewidths of pump and signal (idler) resonances can be engineered independently. A high spectral purity of 95 % ± 1.5 % is obtained via a time-integrated g ( 2 ) correlation measurement, which exceeds the theoretical 93% bound of a traditional ring’s spontaneous four-wave-mixing photon source. This source also possesses high performance in other metrics including a measured coincidence of 9599 pairs/s and a preparation heralding efficiency of 52.4% at a relatively low pump power of 61 µW as well as high drop-to-through suppression of 20.2 dB. By overcoming the trade-off between spectral purity and brightness in the post-filtering way, such a method guarantees bright pure photons and will pave the way for development of on-chip quantum information processing with improved operation fidelity and efficiency.
Single-photon purity is one of the most important key metrics of many quantum states of light. For applications in photonic quantum technologies, e.g. quantum communication and linear optical quantum computing, a minimization of the multi-photon error rate is required because of its error-introducing nature. Ultimately, the purity of state-of-the-art single-photon sources was found to be limited by spontaneous emission and subsequent reexcitation during the interaction with the driving field. Here, we demonstrate that even this fundamental limit to the single-photon purity can be overcome due to the distinct spectro-temporal properties of the individual photons forming multi-photon errors. For driving pulses shorter than the emitter lifetime, we find that photons emitted during the pulse exhibit a significantly broader spectral shape than the emitter's natural linewidth. Thus, we can selectively filter out the majority of this instantaneously emitted photon by employing narrowband spectral filters, which reduces the measured degree of second-order coherence at zero time delay by almost one order of magnitude. This enables a significant suppression of the multi-photon error rate without detrimental effects on the desired single-photon emission.