• Photonics Research
  • Vol. 5, Issue 4, 324 (2017)
Yuanhua Li1、2, Tong Xiang1、2, Yiyou Nie3, Minghuang Sang3, and Xianfeng Chen1、2、*
Author Affiliations
  • 1State Key Laboratory of Advanced Optical Communication Systems and Networks, Department of Physics and Astronomy, Shanghai Jiao Tong University, Shanghai 200240, China
  • 2Key Laboratory for Laser Plasma (Ministry of Education), Collaborative Innovation Center of IFSA (CICIFSA), Shanghai Jiao Tong University, Shanghai 200240, China
  • 3Department of Physics, Jiangxi Normal University, Nanchang 330022, China
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    DOI: 10.1364/PRJ.5.000324 Cite this Article Set citation alerts
    Yuanhua Li, Tong Xiang, Yiyou Nie, Minghuang Sang, Xianfeng Chen. Nonlinear interaction between broadband single-photon-level coherent states[J]. Photonics Research, 2017, 5(4): 324 Copy Citation Text show less
    Experimental setup. A mode-locked optical fiber laser generates 500 fs pulses at 1551 nm with a repetition of 59.98 MHz and is used to generate the two chirped broadband single-photon-level coherent states based on FBG1 and FBG2. The two chirped broadband coherent states are combined via a 50∶50 single-mode beam splitter (SBS) and directed to a 5.2 cm long fiber pigtailed Type-0 PPLN-WG chip. The total losses in the WG are 2.2 dB, such as a coupling loss of about 0.7 dB and a total fiber-to-output-facet loss of approximately 1.5 dB. The unconverted photons are deterministically separated from the SFG photons by an IF, and the SFG photons are sent to a single photon detector (silicon APD). The entire experiment is fiber-coupled.
    Fig. 1. Experimental setup. A mode-locked optical fiber laser generates 500 fs pulses at 1551 nm with a repetition of 59.98 MHz and is used to generate the two chirped broadband single-photon-level coherent states based on FBG1 and FBG2. The two chirped broadband coherent states are combined via a 5050 single-mode beam splitter (SBS) and directed to a 5.2 cm long fiber pigtailed Type-0 PPLN-WG chip. The total losses in the WG are 2.2 dB, such as a coupling loss of about 0.7 dB and a total fiber-to-output-facet loss of approximately 1.5 dB. The unconverted photons are deterministically separated from the SFG photons by an IF, and the SFG photons are sent to a single photon detector (silicon APD). The entire experiment is fiber-coupled.
    (a) Pump and signal light spectrums. (b) Spectrums of upconverted light (SFG and SHG): SHG of signal light; SHG of pump light.
    Fig. 2. (a) Pump and signal light spectrums. (b) Spectrums of upconverted light (SFG and SHG): SHG of signal light; SHG of pump light.
    SFG efficiency. SFG efficiency can be tuned by manipulating the PPLN-WG chip’s temperature.
    Fig. 3. SFG efficiency. SFG efficiency can be tuned by manipulating the PPLN-WG chip’s temperature.
    SFG efficiency and SFG photons that the pump photons are upconverted when interacting with the signal photons inside the PPLN-WG chip, plotted against the number of photons per pulse (equal for signal and pump). Dark counts of 3.8 Hz have been subtracted, and the total losses of about 5.6 dB have been taken into account.
    Fig. 4. SFG efficiency and SFG photons that the pump photons are upconverted when interacting with the signal photons inside the PPLN-WG chip, plotted against the number of photons per pulse (equal for signal and pump). Dark counts of 3.8 Hz have been subtracted, and the total losses of about 5.6 dB have been taken into account.
    Yuanhua Li, Tong Xiang, Yiyou Nie, Minghuang Sang, Xianfeng Chen. Nonlinear interaction between broadband single-photon-level coherent states[J]. Photonics Research, 2017, 5(4): 324
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