2019
DOI: 10.1038/s41586-019-1709-y
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A gated quantum dot strongly coupled to an optical microcavity

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Cited by 209 publications
(172 citation statements)
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“…Assuming that the slight increase in broadening with respect to the transform limit arises solely from charge noise, the linewidth measurement places an upper bound of~3.0 Vcm −1 for the root-mean-square (rms) electric field noise at the location of QD1. This upper bound is comparable to the best gated InGaAs QD devices 20,29,40,42,43 . For applications as single-photon source, it is crucial to demonstrate that the photons are emitted one by one, i.e., photon anti-bunching.…”
Section: Resultsmentioning
confidence: 61%
See 1 more Smart Citation
“…Assuming that the slight increase in broadening with respect to the transform limit arises solely from charge noise, the linewidth measurement places an upper bound of~3.0 Vcm −1 for the root-mean-square (rms) electric field noise at the location of QD1. This upper bound is comparable to the best gated InGaAs QD devices 20,29,40,42,43 . For applications as single-photon source, it is crucial to demonstrate that the photons are emitted one by one, i.e., photon anti-bunching.…”
Section: Resultsmentioning
confidence: 61%
“…Applied to a droplet GaAs QD, such techniques could prolong the spin dephasing time to values several orders of magnitude above the radiative lifetime. In this case, in combination with optical cavities 20 , droplet GaAs QDs can potentially serve as fast, high-fidelity sources of spin-photon pairs and cluster states 21 .…”
mentioning
confidence: 99%
“…Quantum dots (QDs) in nanophotonic structures are excellent sources of single photons [10][11][12][13][14] , and planar waveguides are well suited for scaling up to multiple photons and emitters thanks to near-unity photon-emitter coupling 15 and advanced on-chip functionalities 16 . An ideal single-photon source requires suppressing noise and decoherence, which notably has been demonstrated in electrically contacted heterostructures [17][18][19][20] through resonant optical excitation. However, resonant optical excitation is challenging to implement experimentally as it requires suppressing the excitation laser (same frequency as the QD emission) without affecting the source efficiency.…”
mentioning
confidence: 99%
“…In parallel to these studies, semiconductor cavity QED systems have shown similar QED phenomena [ 6 ]. Nowadays, the atomic and semiconductor cavity QED systems [ 7 , 8 , 9 ] present several applications in quantum computing to conceive quantum gates and networks [ 10 ]. In particular, spatially separated qubits are proposed as potential physical realization for quantum networks [ 11 , 12 , 13 , 14 , 15 , 16 , 17 ].…”
Section: Introductionmentioning
confidence: 99%