2019
DOI: 10.1038/s41563-019-0418-0
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Scalable in operando strain tuning in nanophotonic waveguides enabling three-quantum-dot superradiance

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Cited by 128 publications
(87 citation statements)
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“…Another opportunity is to scale-up the circuit so that one excitation pulse could be pumping multiple QDs in parallel. In order to overcome the spectral inhomogeneity of QDs, such a device will require independent tunability of the different QDs to match the frequency of the excitation pulse 39,40 . With such an approach with the circuit, the benefits of the scalable planar platform will be fully exploited in the ongoing pursuit of scaling up single-photon technology 41 .…”
Section: Discussionmentioning
confidence: 99%
“…Another opportunity is to scale-up the circuit so that one excitation pulse could be pumping multiple QDs in parallel. In order to overcome the spectral inhomogeneity of QDs, such a device will require independent tunability of the different QDs to match the frequency of the excitation pulse 39,40 . With such an approach with the circuit, the benefits of the scalable planar platform will be fully exploited in the ongoing pursuit of scaling up single-photon technology 41 .…”
Section: Discussionmentioning
confidence: 99%
“…We show in Fig.2d that our device is compatible with the use of electrical Starktuning, to control the wavelength of individual QD transitions. This is of particular interest for extending recent demonstrations of few-QD interactions in waveguide QED [30,31] to the chiral regime supported by topological interfaces. Furthermore, we employ a Hanbury Brown and Twiss measurement to show clear single photon emission from a QD in the topological waveguide (see Fig.2e), with a g (2) (0) value of 0.09 ± 0.08 (after deconvolution of the instrument response).…”
Section: A Topological Waveguide Operationmentioning
confidence: 94%
“…On the other hand, waveguide architectures that can couple light into and out of remotely located quantum emitters could be ideal. Such a platform offers high extraction efficiency, significant Purcell enhancement, charge control, the ability for local strain tuning, and the freedom to guide light anywhere on chip to and from randomly positioned QDs [20,21]. However, the generation of high-visibility two-photon interference from remote QDs is a significant challenge to be met in all approaches [60][61][62].…”
Section: Discussion and Outlookmentioning
confidence: 99%
“…Visions of fully integrated quantum photonic chips, which require on-demand indistinguishable single-photon generation integrated on chip with low-loss directional couplers, phase shifters, filters, and singlephoton detectors, have been presented [1][2][3][4]. On-chip integration of solid-state emitters such as color centers in diamond [5][6][7][8], molecules [9,10], two-dimensional materials [11][12][13][14], and III-V semiconductor quantum dots (QDs) [15][16][17][18][19][20][21], are particularly promising for these applications. As solid-state emitters reach maturity, the next logical step is to interface these sources with larger quantum photonic architectures to promote the scalability and realization of multipartite quantum-information protocols [22].…”
Section: Introductionmentioning
confidence: 99%