Towards optimal single-photon sources from polarized microcavities

An optimal single-photon source should deterministically deliver one and only one photon at a time, with no trade-off between the source's efficiency and the photon indistinguishability. However, all reported solid-state sources of indistinguishable single photons had to rely on polarization fi...

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Veröffentlicht in:arXiv.org 2019-07
Hauptverfasser: Wang, Hui, Yu-Ming, He, Chung, Tung Hsun, Hu, Hai, Yu, Ying, Chen, Si, Ding, Xing, Ming-Cheng, Chen, Qin, Jian, Yang, Xiaoxia, Liu, Run-Ze, Zhao-Chen, Duan, Jin-Peng, Li, Gerhardt, Stefan, Winkler, Karol, Jurkat, Jonathan, Lin-Jun, Wang, Gregersen, Niels, Yong-Heng Huo, Dai, Qing, Yu, Siyuan, Hoefling, Sven, Chao-Yang, Lu, Jian-Wei, Pan
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Sprache:eng
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Zusammenfassung:An optimal single-photon source should deterministically deliver one and only one photon at a time, with no trade-off between the source's efficiency and the photon indistinguishability. However, all reported solid-state sources of indistinguishable single photons had to rely on polarization filtering which reduced the efficiency by 50%, which fundamentally limited the scaling of photonic quantum technologies. Here, we overcome this final long-standing challenge by coherently driving quantum dots deterministically coupled to polarization-selective Purcell microcavities--two examples are narrowband, elliptical micropillars and broadband, elliptical Bragg gratings. A polarization-orthogonal excitation-collection scheme is designed to minimize the polarization-filtering loss under resonant excitation. We demonstrate a polarized single-photon efficiency of 0.60+/-0.02 (0.56+/-0.02), a single-photon purity of 0.975+/-0.005 (0.991+/-0.003), and an indistinguishability of 0.975+/-0.006 (0.951+/-0.005) for the micropillar (Bragg grating) device. Our work provides promising solutions for truly optimal single-photon sources combining near-unity indistinguishability and near-unity system efficiency simultaneously.
ISSN:2331-8422
DOI:10.48550/arxiv.1907.06818