• Advanced Photonics
  • Vol. 5, Issue 3, 036003 (2023)
Ji-Ning Zhang1、2、3, Ran Yang1、2、3, Xinhui Li1、2、3、*, Chang-Wei Sun1、2、3, Yi-Chen Liu1、3、4, Ying Wei1、2、3, Jia-Chen Duan1、2、3, Zhenda Xie1、3、5, Yan-Xiao Gong1、2、3、6、*, and Shi-Ning Zhu1、2、3
Author Affiliations
  • 1Nanjing University, National Laboratory of Solid State Microstructures, Nanjing, China
  • 2Nanjing University, School of Physics, Nanjing, China
  • 3Nanjing University, Collaborative Innovation Center of Advanced Microstructures, Nanjing, China
  • 4Qingdao University of Technology, School of Science, Qingdao, China
  • 5Nanjing University, School of Electronic Science and Engineering, Nanjing, China
  • 6Hefei National Laboratory, Hefei, China
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    DOI: 10.1117/1.AP.5.3.036003 Cite this Article Set citation alerts
    Ji-Ning Zhang, Ran Yang, Xinhui Li, Chang-Wei Sun, Yi-Chen Liu, Ying Wei, Jia-Chen Duan, Zhenda Xie, Yan-Xiao Gong, Shi-Ning Zhu. Realization of a source-device-independent quantum random number generator secured by nonlocal dispersion cancellation[J]. Advanced Photonics, 2023, 5(3): 036003 Copy Citation Text show less
    Experimental setup of the source-DI QRNG. (a) Entanglement source: the time–energy entangled photon pairs are generated from the Ti:PPLN waveguide pumped by a pulsed laser with a duration of 5 ns, which are separated by a PBS. (b) Measurement device: photons are passively selected for measurement Tδ or Dδ by a 90:10 beam splitter (BS) after being coupled to fiber in Alice and Bob sides. PC, polarization controller; FI, filter; C-BG, chirped Bragg grating; OC, optical circulator; SNSPD, superconducting nanowire single-photon detector; and TDC, time-to-digital converter.
    Fig. 1. Experimental setup of the source-DI QRNG. (a) Entanglement source: the time–energy entangled photon pairs are generated from the Ti:PPLN waveguide pumped by a pulsed laser with a duration of 5 ns, which are separated by a PBS. (b) Measurement device: photons are passively selected for measurement Tδ or Dδ by a 90:10 beam splitter (BS) after being coupled to fiber in Alice and Bob sides. PC, polarization controller; FI, filter; C-BG, chirped Bragg grating; OC, optical circulator; SNSPD, superconducting nanowire single-photon detector; and TDC, time-to-digital converter.
    Photon coincidence counts (CCs) recorded for four measurement combinations of two observers (denoted as A and B) in 10 s.
    Fig. 2. Photon coincidence counts (CCs) recorded for four measurement combinations of two observers (denoted as A and B) in 10 s.
    Smooth entropy Hlowϵ(TδA|E)ρ with respect to the frame size Nd for different processing units NTA. The dotted lines represent the entropy evaluated from the experimental data. The red triangles represent optimal results.
    Fig. 3. Smooth entropy Hlowϵ(TδA|E)ρ with respect to the frame size Nd for different processing units NTA. The dotted lines represent the entropy evaluated from the experimental data. The red triangles represent optimal results.
    Autocorrelation coefficients of raw random data and final random data.
    Fig. 4. Autocorrelation coefficients of raw random data and final random data.
    Results of NIST statistical test suite.
    Fig. 5. Results of NIST statistical test suite.
    Refs.Uncharacterized SourceUncharacterized MeasurementFinite-size AnalysisFinite Measurement Ranges ConsideredaGeneration Rate
    15××5.7 kbps
    17××47.8 Mbps
    20×1 Mbps
    21××8.05 Gbps
    24×b1 Mbps
    25c23 bps
    27d1.25 Mbps
    31××17 Gbps
    This work×4 Mbps
    Table 1. Features of our protocol as compared to the features of existing semi-DI QRNG protocols.
    Ji-Ning Zhang, Ran Yang, Xinhui Li, Chang-Wei Sun, Yi-Chen Liu, Ying Wei, Jia-Chen Duan, Zhenda Xie, Yan-Xiao Gong, Shi-Ning Zhu. Realization of a source-device-independent quantum random number generator secured by nonlocal dispersion cancellation[J]. Advanced Photonics, 2023, 5(3): 036003
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