• Photonics Research
  • Vol. 7, Issue 3, A1 (2019)
Yan Liang1、3, Qilai Fei1, Zhihe Liu1, Kun Huang1, and Heping Zeng1、2、*
Author Affiliations
  • 1Shanghai Key Laboratory of Modern Optical Systems, Engineering Research Center of Optical Instruments and Systems, Ministry of Education, School of Optical-Electrical and Computer Engineering, University of Shanghai for Science and Technology, Shanghai 200093, China
  • 2State Key Laboratory of Precision Spectroscopy, East China Normal University, Shanghai 200062, China
  • 3e-mail: yanliangSPD@163.com
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    DOI: 10.1364/PRJ.7.0000A1 Cite this Article Set citation alerts
    Yan Liang, Qilai Fei, Zhihe Liu, Kun Huang, Heping Zeng. Low-noise InGaAs/InP single-photon detector with widely tunable repetition rates[J]. Photonics Research, 2019, 7(3): A1 Copy Citation Text show less
    Schematic setup of the InGaAs/InP SPD with ultrashort gates. SG, signal generator; LD, laser diode; Attn1, variable optical attenuator; PG, pulse-generating module; Cap, adjustable capacitor; PS, phase shifter; Attn2, variable electric attenuator; MTNT, so-called magic-T network consisting of a broadband transformer; LPF, low-pass filter; AMP: RF amplifier; OSC, oscilloscope. Inset, waveform of 1-GHz signal output of the PG.
    Fig. 1. Schematic setup of the InGaAs/InP SPD with ultrashort gates. SG, signal generator; LD, laser diode; Attn1, variable optical attenuator; PG, pulse-generating module; Cap, adjustable capacitor; PS, phase shifter; Attn2, variable electric attenuator; MTNT, so-called magic-T network consisting of a broadband transformer; LPF, low-pass filter; AMP: RF amplifier; OSC, oscilloscope. Inset, waveform of 1-GHz signal output of the PG.
    (a)–(c) Oscilloscope trace of the output of the APD, the MTNT, and the RF amplifier, respectively; (d) and (e) frequency spectrum of the output of the MTNT and the RF amplifier, respectively.
    Fig. 2. (a)–(c) Oscilloscope trace of the output of the APD, the MTNT, and the RF amplifier, respectively; (d) and (e) frequency spectrum of the output of the MTNT and the RF amplifier, respectively.
    (a) Waveforms of the amplified output signal of the MTNT and LPF at 100 MHz captured by the oscilloscope in the single mode; (b) DCR and AP as functions of DE of the SPD at 100 MHz.
    Fig. 3. (a) Waveforms of the amplified output signal of the MTNT and LPF at 100 MHz captured by the oscilloscope in the single mode; (b) DCR and AP as functions of DE of the SPD at 100 MHz.
    (a) Waveforms of the amplified output signal of the MTNT and LPF at 700 MHz captured by the oscilloscope in the single mode; (b) DCR and AP as functions of DE of the SPD at 700 MHz.
    Fig. 4. (a) Waveforms of the amplified output signal of the MTNT and LPF at 700 MHz captured by the oscilloscope in the single mode; (b) DCR and AP as functions of DE of the SPD at 700 MHz.
    (a) and (b) DCR and AP as functions of DE of the SPD at 1 and 1.25 GHz; (c) count rate dependent on the laser pulse delay.
    Fig. 5. (a) and (b) DCR and AP as functions of DE of the SPD at 1 and 1.25 GHz; (c) count rate dependent on the laser pulse delay.
     DE of 10%DE of 20%
    FrepDCR (×106/gate)APDCR (×106/gate)AP
    100 MHz0.41.9%0.95.3%
    700 MHz0.73.7%3.315.7%
    1 GHz0.81.2%2.54.1%
    1.25 GHz1.11.4%3.24.5%
    Table 1. Performance of the SPD at Different Repetition Frequencies
    Yan Liang, Qilai Fei, Zhihe Liu, Kun Huang, Heping Zeng. Low-noise InGaAs/InP single-photon detector with widely tunable repetition rates[J]. Photonics Research, 2019, 7(3): A1
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